BURST-MODE FOR LOW POWER OPERATION OF RF FLUORESCENT LAMPS

Abstract

An RF fluorescent lamp comprising an electric ballast comprising an inverter circuit operating at a first frequency that provides the voltage and current with reference to local ground to a switching node connected to a first end of a winding of a power coupler, a timing circuit operating at a second frequency equal to or less than half the first frequency, and an enable circuit activated by the timing circuit that enables and disables the inverter circuit.

Description

CROSS-REFERENCE TO RELATED APPLICATIONS

This patent application is related to the following patent applications: U.S. patent application Ser. No. 15/671,520, filed Aug. 8, 2017 (LCDY-0039-U01); U.S. patent application Ser. No. 14/476,189, filed Sep. 3, 2014 (LCDY-0038-U01-C01); U.S. patent application Ser. No. 14/339,091, filed Jul. 23, 2014 (LCDY-0038-U01; U.S. patent application Ser. No. 14/042,598, filed Sep. 30, 2013 (LCDY-0037-U01); U.S. patent application Ser. No. 14/042,580, filed Sep. 30, 2013 (LCDY-0034-U01), now U.S. Pat. No. 9,524,861; U.S. patent application Ser. No. 14/039,066, filed Sep. 27, 2013 (LCDY-0017-U01), now U.S. Pat. No. 9,305,765; U.S. patent application Ser. No. 14/030,758, filed Sep. 18, 2013 (LCDY-0014-U01); U.S. patent application Ser. No. 14/016,363, filed Sep. 3, 2013 (LCDY-0015-U01); U.S. patent application Ser. No. 13/968,766, filed Aug. 16, 2013 (LCDY-0013-U01); U.S. patent application Ser. No. 13/957,846, filed Aug. 2, 2013 (LCDY-0006-U01); U.S. patent application Ser. No. 13/837,034 filed Mar. 15, 2013 (LCDY-0003-U01), now U.S. Pat. No. 9,161,422; U.S. patent application Ser. No. 13/684,664 filed Nov. 26, 2012 (LCDY-0002-U01); U.S. patent application Ser. No. 13/684,665 filed Nov. 26, 2012 (LCDY-0002-U02), now U.S. Pat. No. 8,698,413; U.S. patent application Ser. No. 13/684,660 filed Nov. 26, 2012 (LCDY-0001-U01), now U.S. Pat. No. 8,872,426; U.S. Provisional Patent Application Ser. No. 61/874,401, filed Sep. 6, 2013 (LCDY-0014-P01); and U.S. Provisional Patent Application Ser. No. 61/863,171, filed Aug. 7, 2013 (LCDY-0012-P01).

All of the above patent applications and patents are incorporated herein by reference in their entirety.

BACKGROUND

Field

The present invention relates generally to RF fluorescent light bulbs.

Description of Related Art

Discharge lamps create light by exciting an electrical discharge in a gas and using that discharge to create visible light in various ways. In the case of fluorescent lamps the gas is typically a mixture of argon, krypton and/or neon, plus a small amount of mercury. Other types of discharge lamps may use other gasses. The gas is contained in a partially evacuated envelope, typically transparent or translucent, typically called a bulb or arc tube depending upon the type of lamp.

In conventional discharge lamps the electrically conductive electrodes mounted inside the bulb or arc tube along with the gas provide the electric field used to drive the discharge.

Use of electrodes can create certain problems. First, the discharge is typically designed to have a relatively high voltage in order to minimize losses at the electrodes. In the case of fluorescent lamps, this may lead to long, thin lamp structures, which function well for lighting office ceilings, but are not always a good fit for replacing conventional incandescent lamps. Fluorescent lamps designed to replace incandescent lamps, known as compact fluorescent lamps, or CFLS, are typically constructed by bending the long, thin tube, such as into multiple parallel tubes or into a spiral, which is now the most common form of CFLS. A plastic cover shaped like a conventional incandescent lamp is sometimes placed over the bent tubes to provide a more attractive shape, but these covers absorb light, making the lamp less efficient. Bent and spiral tube lamps also have wasted space between the tubes, making them larger than necessary. The use of a cover increases the size further.

The use of electrodes can create problems other than shape and size. Electrodes can wear out if the lamp is turned on and off many times, as is typical in a residential bathroom and many other applications. The life of the electrodes can also be reduced if the lamp is dimmed, because the electrodes are preferably operated in a specific temperature range and operation at different power levels can cause operation outside the preferred ranges, such as when operating at lower power, which can allow the electrodes to cool below the specified temperature range.

In addition, the long thin shape selected, because it is adapted to allow use of electrodes, tends to require time for mercury vapor to diffuse from one part of the tube to another, leading to the long warm-up times typically associated with many compact fluorescent lamps.

Finally, the electrodes are normally designed to be chemically compatible with the gas used in the lamp. While this is not usually a concern with typical fluorescent lamps, it can be a problem with other types of discharge lamps.

One way to avoid the problems caused by electrodes is to make a lamp that does not use electrodes, a so-called electrodeless lamp. In an electrodeless lamp, the discharge may be driven by, for example, 1) an electric field created by electrodes mounted outside the bulb or arc tube; 2) an electric field created by a very high frequency electromagnetic field, usually in combination with a resonant cavity, or 3) an electric field created by a high frequency magnetic field without the use of a resonant cavity. This latter lamp is called an induction-coupled electrodeless lamp, or just “induction lamp.”

In an induction lamp, a high frequency magnetic field is typically used to create the electric field in the lamp, eliminating the need for electrodes. This electric field then powers the discharge.

Since induction lamps do not require use of electrodes, they do not need to be built into long thin tubes. In fact, a ball-shaped bulb, such as the bulb used for conventional incandescent lamps, is a preferred shape for an induction lamp. In addition, since induction lamps do not use electrodes, they can be turned on and off frequently without substantial adverse impact on loss of life. The absence of electrodes also means that induction lamps can be dimmed without reducing lamp life. Finally, the ball-shaped lamp envelope allows rapid diffusion of mercury vapor from one part of the lamp to another. This means that the warm-up time of induction lamps is typically much faster than the warm-up time of most conventional compact fluorescent lamps.

Induction lamps fall into two general categories, those that use a “closed” magnetic core, usually in the shape of a torus, and those that use an “open” magnetic core, usually in the shape of a rod. Air core induction lamps fall into this latter category. Closed core lamps are usually operated at frequencies generally above 50 kHz, while open core lamps usually require operating frequencies of 1 MHz and above for efficient operation. The lower operating frequency of closed core induction lamps makes them attractive; however, the bulb design required to accommodate the closed core makes them generally unsuitable for replacing standard in incandescent lamps. Open core induction lamps, while requiring higher operating frequencies, allow the design of lamps that have the same shape and size as common household incandescent lamps. This disclosure is primarily is addressed to the open core category of induction lamps.

In spite of their obvious advantages, there are very few open core induction lamps on the market today. One reason for the lack of commercially successful products is the cost of the high frequency ballast. Conventional fluorescent lamps, including CFLS, can be operated at frequencies from 25 kHz to 100 kHz, a frequency range where low cost ballast technology was developed in the 1990s, and closed core induction lamps can be operated at frequencies from 50 kHz to 250 kHz, for which the ballasts are only slightly more expensive. However, open core induction lamps typically require operating frequencies of 1 MHz or higher. The United States Federal Communications Commission (FCC) has established a “lamp band” between 2.51 MHz and 3.0 MHz that has relaxed limits on the emission of radio frequency energy that may interfere with radio communication services. Cost effective open core induction lamps may preferably have an operating frequency of at least 2.51 MHz.

The lack of commercially successful open core induction lamps may be traced to the absence of a low-cost ballast that can operate in the 2.51 MHz to 3.0 MHz band while meeting all the requirements of the FCC; that is small enough to fit into a lamp; that has a ballast housing that is the same size and shape as a conventional incandescent lamp; and that can be dimmed on conventional TRIAC dimmers found in homes in certain major markets, such as the U.S. The present disclosure addresses one or more of these issues. Therefore, a need exists for improved induction lamps, especially in residential applications.

SUMMARY

In accordance with exemplary and non-limiting embodiments, systems and methods for the configuration and operation of an electrodeless lamp, also referred to as an induction lamp, are provided. One or more certain aspects may be incorporated in certain embodiments.

In embodiments, an aspect of the lamp is burst-mode inverter operation to maintain stability at low power, where a timing circuit synchronously enables-disables the higher-frequency inverter, rapidly turning the lamp on and off with off-times that are short enough that the plasma doesn't have enough time to dissipate completely while the inverter is disabled.

In embodiments, an aspect of the lamp utilizes a pulsed operation and is further improved through the use of a fast turn-on circuit.

In embodiments, an aspect of the lamp utilizes a pulsed operation and is further improved through the use of a high-Q coupler core for improved efficiency through fast re-strike at elevated coupler voltage amplitude.

In embodiments, an aspect of the lamp utilizes a layered metal-oxide coating in association with phosphor coating of the lamp's vitreous envelope to improve lumen maintenance.

In embodiments, an aspect of the lamp comprises a vitreous portion with a burner envelop with a remote glass sealing configuration.

In embodiments, an aspect of the lamp is an RF induction lamp with a bulbous vitreous portion of the RF fluorescent lamp comprising a vitreous envelope filled with a working gas mixture that has the outward appearance of a G25 incandescent bulb.

In embodiments, an aspect of the lamp is an RF induction lamp with improved EMI containment through multiple EMI shields mounted in association with ballast electronics boards.

In embodiments, an aspect of the lamp is an RF induction lamp with improved thermal management through the use of a heat spreader in association with ballast electronics boards.

In embodiments, an aspect of the lamp utilizes UV light sources (alone or in combination with visible light sources) to excite phosphor coatings, such as other than through mercury plasma discharge.

In embodiments, an aspect of the lamp utilizes multiple burners into the induction lamp, such as to provide cool temperature selection.

BRIEF DESCRIPTION OF THE FIGURES

The invention and the following detailed description of certain embodiments thereof may be understood by reference to the following figures:

FIG. 1 depicts a high-level functional block diagram of an embodiment of the induction lamp.

FIG. 1A depicts embodiment dimensionality for an induction lamp.

FIG. 1B depicts embodiment dimensionality for an induction lamp.

FIG. 2 shows a typical circuit diagram of a TRIAC based dimmer known in the art.

FIG. 3 shows a block diagram of an electronic ballast without an electrolytic smoothing capacitor known in the art.

FIG. 4 illustrates dimming operation of the electronic ballast known in the art.

FIG. 5 shows a block diagram of an electronic ballast with a dimming arrangement in accordance with the present invention.

FIG. 6 illustrates the ballast and lamp operation method in accordance with an exemplary embodiment.

FIG. 7 shows a block-schematic diagram of the TRIAC dimmed ballast according to an exemplary embodiment.

FIG. 8 shows a block-circuit diagram according to an exemplary embodiment.

FIG. 9 shows oscillograms of the TRIAC voltage, lamp current and lamp voltage in a dimming mode, according to an exemplary embodiment.

FIG. 10 shows an embodiment for a pass-through circuit.

FIG. 11 depicts an exemplary embodiment cross-section view of an RF induction lamp.

FIG. 12 depicts an exemplary embodiment cross-section view of a coupler with the inserted grounded shell.

FIG. 12A depicts an exemplary embodiment of a capacitor acting to provide electrical isolation from a ferrite core coupler.

FIG. 12B depicts an exemplary embodiment of a capacitor acting to provide electrical isolation from an air-core coupler

FIG. 13 shows an exemplary experimental and commercial lamp covered with copper foil for purposes of an experiment.

FIG. 14 illustrates an exemplary experimental set-up for measurement of the lamp surface voltage.

FIG. 15 provides experimental data of conductive EMI (points) and the allowed limits (lines) taken with a related art lamp using a LISN set up.

FIG. 16 provides experimental data of conductive EMI (points) and the allowed limits (lines) taken with the test lamp accordance to an exemplary and non-limiting embodiment.

FIG. 17 shows a block-circuit diagram of electronic ballast comprising a Passive Valley Fill PF correction circuit accordingly to the present invention.

FIG. 18 shows waveforms of the input current and DC bus voltage of the ballast in FIG. 17.

FIG. 19 shows a block-circuit diagram of electronic ballast with a Passive Valley Fill Circuit dimmed by TRIAC based dimmer.

FIG. 20 shows waveforms of the input current and DC bus voltage of the ballast in FIG. 19.

FIG. 21 provides an EMI reduction embodiment where a conductive material in contact with the ferromagnetic core of the power coupler is wrapped from the inside of the core to the outside of the windings on the core.

FIG. 22A shows a method of attaching the flag.

FIG. 22B shows a method of attaching the flag.

FIG. 22C shows two flag orientations.

FIG. 22D shows a folded flag in two different orientations.

FIG. 22E shows a folded flag and a starting in aid in two different orientations.

FIG. 23 shows a Paschen-like curve.

FIG. 24 shows an example of a high frequency DC-to-AC inverter circuit.

FIG. 25 shows an example of a DC-to-AC inverter with a matching network.

FIG. 26 shows an example of a DC-to-AC inverter with a matching network.

FIG. 27 shows an example of a DC-to-AC inverter with a matching network.

FIG. 28 shows an example of a DC-to-AC inverter with a matching network.

FIG. 29 shows an example of a DC-to-AC inverter with a matching network.

FIGS. 30A-B show examples of a bent wire mount.

FIG. 31A-B show examples of a helix mount.

FIG. 32A-B show examples of an alternate helix mount

FIG. 33-34 shows different spacing of coupler windings.

FIG. 35 shows a printed circuit board with vertically mounted components.

FIG. 36 shows an example of a heat spreader.

FIG. 37 shows an example of heat spreader in contact with the upright electrical components.

FIG. 38 shows an example of a clip.

FIG. 39 shows a printed circuit board with a clip holding the heat spreader in contact with certain electrical components.

FIG. 40 depicts a magnetic field generated by a closely wound solenoid.

FIG. 41 depicts an exemplary embodiment of an induction lamp having three wires wound in parallel on the coupler core.

FIG. 42A depicts an exemplary embodiment of an induction lamp where the winding on the core has variable spacing, being more closely wound in the middle of the core relative to the winding spacing at the ends of the core.

FIG. 42B depicts an exemplary embodiment of an induction lamp where the winding on the core has variable spacing, being more closely wound at the ends of the core relative to the winding spacing at the center of the core.

FIG. 43 depicts an exemplary embodiment of an induction lamp where the end of the RF source that is not connected to circuit common is electrically connected to the turns of wire along the coupler at the end farthest from the ballast.

FIG. 44 depicts the relationship between mercury vapor pressure within lamp envelope and luminous output.

FIG. 45 depicts a system for evaluating amalgam composition.

FIG. 46 depicts the amalgam performance measurement process.

FIG. 47 illustrates characteristic light output measurement curves for different mercury vapor pressures.

FIG. 48 depicts an exemplary embodiment of dimensionality for an induction lamp.

FIG. 49A depicts an exemplary embodiment of an internal configuration for an induction lamp.

FIG. 49B depicts an exemplary embodiment of internal configuration for an induction lamp.

FIG. 50 depicts an exemplary embodiment of a flareless finger for an induction lamp envelope.

FIG. 51 depicts an exemplary embodiment of a coating structure for an induction lamp envelope.

FIG. 52 depicts an exemplary embodiment of a functional block diagram for a pulsed induction lamp.

FIG. 53 depicts an exemplary embodiment of a circuit diagram for a pulsed induction lamp.

FIG. 54 depicts an exemplary embodiment of a switching diagram for a pulsed induction lamp.

FIG. 55 depicts an exemplary embodiment of a diagram for a pulsed induction lamp.

FIG. 56A-E depict an exemplary embodiment of an oscillator circuit diagrams for a pulsed induction lamp.

FIG. 57 depicts an exemplary embodiment of a charge pump circuit diagram for a pulsed induction lamp.

FIG. 58 depicts an exemplary embodiment of a fast startup circuit diagram for a pulsed induction lamp.

FIG. 59 depicts an exemplary embodiment of a restrike diagram for a pulsed induction lamp.

While described in connection with certain exemplary and non-limiting embodiments, other exemplary embodiments would be understood by one of ordinary skill in the art and are encompassed herein. It is therefore understood that, as used herein, all references to an “embodiment” or “embodiments” refer to an exemplary and non-limiting embodiment or embodiments, respectively.

DETAILED DESCRIPTION

An induction-driven electrodeless discharge lamp, hereafter referred to synonymously as an induction lamp, an electrodeless lamp, or an electrodeless fluorescent lamp, excites a gas within a lamp envelope through an electric field created by a time-varying magnetic field rather than through electrically conductive connections (such as electrodes) that physically protrude into the envelope. Since the electrodes are a limiting factor in the life of a lamp, eliminating them potentially extends the life that may be expected from the light source. In addition, because there are no metallic electrodes within the envelope, the burner design may employ high efficiency materials that would otherwise react with the electrodes, such as bromine, chlorine, iodine, and the like, and mixtures thereof, such as sodium iodide and cerium chloride. Embodiments described herein disclose an inductor mounted inside a re-entrant cavity protruding upward within the burner envelope, where the inductor is at least one coil, which may be wound around a core of magnetizable material suitable for operation at the frequency of the time-varying magnetic field, such as ferrite or iron powder, to form the power coupler that creates the time-varying magnetic field that generates the time-varying electric field in the lamp's interior. The power coupler receives electrical power from a high-frequency power supply, known as a ballast, which in embodiments is integrated within the base of the induction lamp. The ballast in turn receives electrical power through a standard base, such as an Edison Screw Base (E39, E26, E17 or E12 base), a GU-24 base, and the like, from the AC mains. The form factor for the induction lamp may take a form similar to a standard incandescent light bulb, (A19 shape) or an incandescent reflector lamp, such as an R30 or BR30, thus allowing it to be used as a replacement for incandescent light bulbs.

Referring to FIG. 1, an embodiment of an induction lamp 100 is illustrated, having an ‘upper’ light providing portion 102 (i.e., the light delivery end, understanding that the lamp may be mounted in any orientation per the lamp socket position), a ‘lower’ electronics portion 104 (i.e. the opposite of the light delivery end), and an electrical-mechanical base connection (e.g. an Edison base), where the proportions and shape of the upper and lower portions of the induction lamp are illustrative, and not meant to be limiting in any way. In embodiments, the upper portion may include the burner envelope 108 with an induction power coupler 110 (comprising winding(s), and optionally a core as described herein) inserted up into a re-entrant cavity 112, where the induction power coupler creates the time-varying magnetic field that, in turn, creates the time-varying electric field within the burner envelop. The burner envelope contains an amalgam that provides mercury vapor. The mercury atoms in the vapor are then both ionized and excited by the time-varying electric field. The excited mercury atoms emit small amounts of visible light plus much larger amounts of ultraviolet energy that is then converted into visible light by a phosphor coating on the inside of the burner envelope, thus the induction lamp provides light to the outside environment.

In embodiments, the external appearance of the upper portion with respect to its optical properties may be similar to traditional phosphor-based lighting devices, where the glass is substantially white due to the phosphor coating on the inside of the envelope. The external appearance of the lower portion with respect to its optical properties may be made to be substantially similar to the upper portion in order to minimize the differences in the appearance of the upper and lower portions, thus minimizing the overall visual differences between the external appearance of the disclosed induction lamp bulb and that of a traditional incandescent bulb, such as having external materials that are similar to the external materials of the upper bulbous portion (e.g. vitreous or vitreous-coated materials).

In embodiments, the induction lamp may be structured with an upper bulbous portion, an electronics portion in the neck or tapered portion of the bulb, a screw base (e.g. Edison base), and the like, where the electronics portion may either show externally as a separate lower portion, such as with the upper portion seated within the neck of the lower portion, or the lower portion may be completely encased within an extended upper portion. That is, the bulbous portion may extend down over the electronics portion as a vitreous envelope all the way to the screw base. In this way, the induction lamp may look nearly identical to an ordinary incandescent light bulb, at least when the induction light bulb is turned on and illuminating, and optionally designed to look the same when illuminated due to an optical design to illuminate down the neck of the induction bulb that is around the electronics portion.

Although FIG. 1, as well as FIGS. 11-12B, shows the electronics (e.g., the ballast) located in the lower portion 104 below the power coupler inside the re-entrant cavity, this is meant to be illustrative, and not limiting, where the electronics may be of a size that fits in a reduced portion of the neck of the bulb, located wholly inside the screw base 138, located inside the reentrant cavity 112, and the like.

Referring to FIG. 1A, the induction lamp may have the approximate shape and dimensions of an ordinary incandescent bulb, with a dimension D_B at the widest point of the bulbous portion 102 being within the NEMA ANSI standards for electric lamps, which sets forth the physical and electrical characteristics of the group of incandescent lamps that have A, G, PS and similar bulb shapes with E26 medium screw bases. The NEMA ANSI C78.20-2003 standard for electric lamps is incorporated herein in its entirety. Although the standard provides the outer most bounds for the specified lamps, the common dimensions for said specified bulbs may be substantially within these ranges. Thus the dimensionality of the induction lamp may be approximately equivalent to those of the ordinary incandescent bulb as manufactured as opposed to the maximum dimensions as specified in the standard, thereby effectively providing a replacement for an ordinary incandescent bulb that matches the user's expectation of the profile and size of an ordinary incandescent bulb.

In an example, and per said referenced NEMA ANSI standard, the maximum for the dimension D_B-A19 at the widest point of the bulbous portion 102 of an A19 bulb is set out to be in the range 68 to 69.5 millimeters. However, in a typical 60 W incandescent A19 bulb D_B-A19 is approximately 60.3 mm (or approximately 2⅜ inches, where ‘A19’ refers to an ‘A’ profile width D_B-A19 of 19 times ⅛ inch). Similarly, the overall length D_H-A19 of an A19 bulb from the bottom of the screw portion to the top of the bulbous portion is specified in the NEMA ANSI standard to be in the range between 100 to 112.7 millimeters for different length versions of the A19 form factor, but the typical 60 W incandescent A19 bulb is approximately 108 millimeters.

In embodiments, the lower portion 104 may take the form of a concave tapering neck that has a maximum tapering diameter DT-A19 substantially less than D_B-A19 into which the upper portion 102 may be seated, such as at an upper-lower interface point 140. The upper-lower interface point 140 may have a maximum diameter where the tapering concave shape of the neck meets the spherical bulbous upper portion 102 that is less than the diameter of the sphere as in an ordinary incandescent bulb, such as approximately 45 mm millimeters plus or minus a tolerance, such as +/−3 mm, +/−2 mm, +/−1 mm, and the like. From the upper-lower interface point 140 the neck may taper in a concave form to the lower-cap interface point 142 at the top of the screw mount 138, such as similar to a typical incandescent bulb. In embodiments, the taper may be such that there is less than a thirty-degree angle between the surface of the lower portion 104 that runs from interface point 142 to 140 and a central axis running through the lamp from the screw mount 138 to the top of the bulbous portion 102. The bulbous portion 102 may be constructed such that it forms a partial sphere having a radius that is one-half of D_B-A19. This may result in the bulbous portion being seated in the neck of the lower portion 104 so that more than a hemisphere of the partial sphere sits above the neck of the lower portion 104. In embodiments, the upper portion 102 and lower portion 104 may be connected in a manner that makes their separation indistinguishable to the viewer, such as by using appropriate overlay or coating materials, or by fashioning a seamless connection between the two portions.

Referring to FIG. 1B, the induction lamp may have the approximate shape and dimensions of an ordinary incandescent bulged reflector bulb, with a dimension D_B-BR30 at the widest point of the bulbous portion 146 being within the NEMA ANSI standards for electric lamps, which sets forth the physical and electrical characteristics of the group of bulk reflector lamps that have BR and similar bulb shapes with E26 medium screw bases. The NEMA ANSI C78.21-2003 standard for electric lamps is incorporated herein in its entirety. Although the standard provides the outer most bounds for the specified lamps, the common dimensions for said specified bulbs may be substantially within these ranges. Thus, the dimensionality of the induction bulged reflector lamp may be approximately equivalent to those of the ordinary bulged reflector bulb as manufactured as opposed to the maximum dimensions as specified in the standard, thereby effectively providing a replacement for an ordinary bulged reflective bulb that matches the user's expectation of the profile and size of an ordinary bulged reflective bulb.

In an example, and per said referenced NEMA ANSI standard, the maximum for the dimension D_B-BR30 at the widest point of the bulbous portion 146 of BR30 bulb is 108.5 millimeters. However, in a typical 65 W incandescent BR30 bulb D_B-BR30 is approximately 95.3 mm (or approximately 3¾ inches, where ‘BR30’ refers to an ‘BR’ profile width D_B-BR30 of 30 times ⅛ inch). Similarly, the overall length D_H-BR30 of a BR30 bulb from the bottom of the screw portion to the top of the bulbous portion is specified in the NEMA ANSI standard to be in the range between 123.8 to 136.5 millimeters for different length versions of the BR30 form factor, but the typical 65 W incandescent BR30 bulb is approximately 129.5-136.5 millimeters (5.13-5.375 inches).

In embodiments, the lower portion 152 may take the form of an approximately vertical rise from the base, DR-BR30, to a minimum height of 46.7 millimeters, which is substantially less than the minimum overall bulb height of 123.8 millimeters. The lower portion 104 may have a maximum diameter DT-BR30 of 43.1 millimeters plus or minus a tolerance, such as +/−3 mm, +/−2 mm, +/−1 mm, and the like. From the upper-lower interface point 144 the bulb may angle up and outward at approximately 540 from the normal to the central axis running through the lamp from the screw mount 138 to the top of the bulbous portion 150 where the sides round radially toward the center of the bulb. At the top of the bulbous portion 150 the lamp may be approximately planar or slightly concave. In embodiments, the upper portion 154 and lower portion 152 may be connected in a manner that makes their separation indistinguishable to the viewer, such as by using appropriate overlay or coating materials, or by fashioning a seamless connection between the two portions.

In embodiments, the electronics to operate the lamp are designed and packaged in such a way that they may be fully contained within the lamp, within the confines of a standard lamp base such as an E26 medium screw base, within the bottom portion 104152 of the lamp bulb, within a re-entrant cavity, and the like. Techniques may include selection of components, including the migration of inductive components to those without ferromagnetic cores, selection of circuit board technology including flexible and printed circuit boards, the use of IC mounting techniques such as flip chip, also known as controlled collapse chip connection, wire bonding, and the like.

In embodiments, the induction lamp may be made to approximate the shape and dimensions for any standard bulb, such that it is better accommodated by lighting fixtures designed for the standard bulb, as well as being generally more familiar to the public, and thus more acceptable as a replacement bulb for commonly used incandescent bulbs. As such, despite the range tolerances provided in the NEMA ANSI standards, the induction lamp may be of a shape that is similar to an ordinary incandescent lamp, such as would be familiar to a member of the public, but with the possibility that a segment exists between the upper bulbous portion 102 and the lower electronics portion 104 as described herein.

In embodiments, other dimensional aspects of the induction lamp may be determined by the selection of a profile and size of the induction bulb to that of a typical incandescent bulb, such as an A19 bulb, a BR30 bulb and the like. For instance, the dimensions of the re-entrant cavity 112 and/or the power coupler 110 may be at least in part determined by the shape and/or size of the bulbous portion 102 of the induction lamp, where the shape of the power coupler 110 as accommodated in the re-entrant cavity 112 determines where the resultant field strength is maximized within the envelope. It may be ideal to have the strength maximized in the plane of the maximum dimension of D_B, such as in the centermost portion of the volume between the re-entrant cavity and the outer wall of the envelope. In this regard, the shape and positioning of the power coupler 110, and the re-entrant cavity 112 it resides in, may include dimensional attributes that improve lamp performance within the dimensional constraints of a typical incandescent bulb.

In embodiments, the induction lamp may include other aspects that contribute to acceptance and compatibility with existing incandescent lighting, such as with dimming compatibility to existing external circuitry (e.g. dimming switches that employ TRIAC or MOSFET switches) and lighting characteristics similar to an incandescent lamp (e.g. brightness level, low flicker, matching color rendering, matching color temperature, and the like). In this way, the induction lamp will substantially resemble a traditional incandescent light bulb, increasing the sense of familiarity of the new induction lamp with the public through association with the incandescent lamp, and thus helping to gain acceptance and greater use for replacement of incandescent light sources.

The induction lamp described in embodiments herein may provide for improved capabilities associated with the design, operation, and fabrication of an induction lamp, including in association with the ballast 114, thermal design 118, dimming 120, burner 122, magnetic induction 124, lighting characteristics 128, bulb characteristics 130, management and control 132, input energy 134, and the like. The ballast, as located in the lower portion of the induction lamp, is the high-frequency power supply that takes mains AC as provided through the base 138, and creates the high-frequency electrical power delivered to the power coupler located in the re-entrant cavity in the upper portion. Improved capabilities associated with the ballast design may include dimming facilities, EMI filter, a rectifier, a power factor correction facility, output driver, circuitry with reduced harmonic distortion, a power savings mode with on-off cycles, lamp start-up, lamp warm-up, power management, and the like. Improved capabilities may provide for a design that provides a compatible thermal environment, such as through a static thermal design, through dynamic power management, and the like.

Improved capabilities associated with the dimming design may include a dimming mechanism, dimming compatibility, a compatible dimming performance relative to a dimming curve, an automatic shutdown circuit, a minimum lumen output, and the like. Dimming capabilities may include methods for dimming and/or TRIAC trigger and holding currents, including frequency dimming, frequency dimming and handshake with TRIAC firing angle, circuits without a traditional smoothing capacitor and with an auxiliary power supply, burst mode dimming, multiple-capacitor off-cycle valley filling circuit, frequency slewing, auto shut-off dimming circuit, current pass-through, utilization of bipolar transistor, holding current pulsed resistor, charge pump, buck or boost converter, and the like.

Improved capabilities associated with the burner design may include aspects related to the size, shape, gas pressure, gas type, phosphor type, materials, EMI reduction via core and/or coupler shielding, methods to reduce light output run-up time, improved lumen maintenance through improved burner processing, use of protective coatings on burner surfaces or improved materials for fabricating the burner envelope and reentrant cavity, and the like.

Improved capabilities associated with the magnetic induction design may include the operating frequency range, electro-magnetic radiation management, reduced electro-magnetic interference utilizing active and passive magnetic induction windings, improved axial alignment through radial spacers, or a grounded shell inserted to the ferromagnetic core, internal transparent conductive coatings, external transparent conductive coating with insulating overcoat, electrical field shield between the coupler and the re-entrant cavity, and the like.

Improved light characteristics provided may include warm-up time, brightness, luminous flux (lumens), flicker, color rendering index, color temperature, lumen maintenance, incandescent-like lighting in a magnetic induction electrodeless lamp, high red rendering index lighting, increased R9, and the like.

Improved lamp characteristics provided may include a bulb base design, globe material, globe shape operating temperature range, bulb temperature, size parameters, instant on electrodeless lamp for residential applications, electrodeless lamp for frequent on/off and motion detector applications, and the like.

Improved capabilities associated with the management and control may include color control, lumen output control, power management, susceptibility to line voltage changes, component variations and/or temperature changes, interaction with other systems, remote control operation (e.g. activation, deactivation, dimming, color rendering), and the like.

Improved capabilities associated with the input source may include AC input voltage, AC input frequency, and other input profile parameters.

Ballast

The ballast is a special power supply that converts power line voltage and current to the voltage and current required to operate the burner. In the U.S. the ballast generally operates from a 120 Volt, 60 Hz AC power line, but the ballast could be designed to operate from AC power lines with different voltages and/or frequencies, or from DC power lines with a range of voltages. Ballasts that are designed for induction-driven electrodeless discharge lamps convert the power line voltage and current into voltage and current with a frequency in the range of 50 kHz to 50 GHz, depending upon the design of the lamp. For the type of induction lamps described in the present disclosure, the ballast output frequency is generally in the 1 MHz to 30 MHz region.

The ballast provides a number of functions in addition to the basic frequency, voltage and current conversion functions. The other key functions include: a) providing a means to generate the high voltages necessary to start the discharge; b) limiting the current that can be delivered to the discharge, and c) reducing the power delivered to the discharge to reduce the light produced when commanded to do so by a user-operated control, i.e., a dimmer.

The conversion from power line voltages and currents to the voltages and currents used to operate the discharge are usually accomplished in a two-step process. In the first step, the power line voltage and current is converted into DC voltage, usually by means of a full wave bridge rectifier and optionally an energy storage capacitor (e.g. an electrolytic storage capacitor to smooth ripple after the rectifier stage). In the second step, the DC power created by the bridge rectifier is converted into high frequency AC power at the desired frequency by means of an inverter. The most common inverter used in discharge lamp ballasts is a half-bridge inverter. Half-bridge inverters are composed of two switches, usually semiconductor switches, connected in series across the DC power bus. The output terminals of the half-bridge inverter are 1) the junction between the two switches, and 2) either side of the DC power bus for the inverter. The half-bridge inverter may be driven by feedback from the matching network described herein or a separate drive circuit. The former is called a “self-oscillating half-bridge inverter” while the latter would be called a “driven half-bridge inverter.”

In addition to half-bridge inverters, the inverter can be configured as a push-pull circuit using two switches, or as a flyback or Class E or other such converter using a single switch.

The switch or switches used for the inverter can be composed of bi-polar transistors, Field Effect Transistors (FETs), or other types of semiconductor switching elements such as TRIACS or Insulated Gate Bi-Polar Transistors (IGBTs), or they can even be composed of vacuum tubes. Ballasts designed for induction lamps generally employ FETs in the inverter.

The output voltage of a half-bridge inverter is typically composed of both DC and AC components. Therefore, at least one DC blocking capacitor is typically connected in series with the induction lamp load when it is connected to the half-bridge inverter. Additionally, a matching network is connected between the output of the half-bridge inverter and the induction-driven lamp load. The matching network provides at least the following four functions: 1) convert the input impedance of the coupler described herein to an impedance that can be efficiently driven by the half-bridge inverter, 2) provide a resonant circuit that can be used to generate the high voltages necessary to initiate the discharge in the burner, 3) provide the current-limiting function that is required by the fact that the discharge has what is known as “negative incremental impedance” which would cause it to draw high levels of current from the half-bridge inverter if that current was not limited by some means, and 4) filter the waveform of the half-bridge inverter, which is generally a square wave, to extract the sine wave at the fundamental frequency of the half-bridge inverter. This last step is necessary to reduce generation by the coupler and burner of electromagnetic radiation at harmonics of the fundamental drive frequency of the half-bridge inverter.

The matching network is typically composed of a resonant circuit that is used to generate high voltage to start the discharge in the burner and then provides the current limiting function after the discharge has been initiated. This resonant circuit is often designed as a series resonant L-C circuit with the lamp connected across the resonant capacitor. However, other configurations are possible. The coupler used with induction lamps is inductive, so the matching network for an induction lamp could be a series C-L with the discharge “connected” across the inductor by virtue of the inductive coupling inherent in such lamps. However, better performance is often achieved with an L-C-L circuit that uses the inductance of the coupler in addition to a separate inductor and capacitor. Other matching networks that employ additional inductors and/or capacitors are known in the art.

Since the half-bridge inverter is operating at a frequency substantially above the power line frequency, it is also generally equipped with what is known as an “EMI filter” where it is connected to the power line. The EMI filter is designed to reduce the level of high frequency noise that the half-bridge inverter injects into the AC power line. To achieve this function, the EMI filter is generally designed as a low pass filter with a cut-off frequency below the operating frequency of the inverter.

In some embodiments, the induction RF fluorescent lamp may operate at higher frequencies, above 2 MHz. These frequencies are achieved using a modified Class E circuit, an example of which is shown in FIG. 24. Class E oscillators and inverters have a maximum theoretical efficiency of 100%, but practical circuits may be limited to an efficiency of 90% to 95% due to losses in the various inductors and capacitors used in the resonant output circuits.

This invention comprises modifications to a Class E circuit. An extra circuit leg, comprising a series-connected inductor, L_MR, 2404 and capacitor, C_MR, 2406, is connected in parallel with the two output terminals of a switching transistor, Q₁, 2410. Additionally, a starting value for the input choke inductor, L_F, 2402, located between the power supply 2412 and the active switch, Q₁, 2410, may be calculated using the following formula:

$L_F=\frac{1}{9{\pi }^2f_s^2C_F}$

where f_s represents the operating frequency and C_F is the device capacitance of the active switch, Q₁, 2410. The above formula represents an initial or starting value for L_F and is not intended to be limiting. The value of the input choke inductor, L_F, 2402 of this invention represents a significant reduction in the value of the input choke inductor relative to that of a typical Class E circuit input choke inductor which typically requires a ferromagnetic core. The reduction in the value of this component may result in the elimination of all ferromagnetic materials from the DC to AC converter section.

The modified Class E circuit of the invention uses a resonant sub-circuit to reduce the peak voltage across the active switch, Q₁, 2410 allowing the use of a higher performance switch such as MOSFET or similar device. With a correct tuning of the resonant sub-circuit, the peak voltage at the active switch, Q₁, 2410 may be reduced relative to a typical Class E circuit by approximately 40%. This allows the use of a lower voltage rated MOSFET and the like. As this is a single transistor circuit, the synchronization issues of a multiple transistor circuit, such as the half bridge inverter and the like, are eliminated. The components of the modified Class E circuit: inductor, L_MR, 2404, capacitor, C_MR, 2406, inductor, L_S, 2412, capacitor, C_S, 2414, and capacitor, C_P, 2416 are selected to achieve low impedance at the 2nd harmonic of the switching frequency and relatively higher inductive impedance at the output of the inverter, the terminals of the active switch, Q₁, 2410 in its off state, at the fundamental frequency of operation; and a capacitive impedance at the 3rd harmonic of the operating frequency at the same pair of nodes. The impedance at the fundamental frequency is larger than the impedance at the 3rd harmonic.

In some embodiments, as shown in FIG. 25, there is a matching network 2502 between the modified Class E circuit of the invention and the circuit load 2420, which is the power coupler for the induction lamp. There are a variety of circuits which may comprise the matching network 2502. FIG. 26 illustrates one example of a matching network 2502 comprising a capacitor, C_M, 2602. FIG. 27 illustrates another example of a matching network 2502 comprising two capacitors, C_M1 2702 and C_M2 2704. FIG. 28 illustrates yet another example of a matching network 2502 comprising two capacitors, C_M1 2802 and C_M2 2804, and an inductor, L_M, 2806. These examples are meant to be illustrative of matching networks 2502 and should not be considered limiting.

At these higher frequencies, the ballast circuit may operate more efficiently as the power level is increased. For instance, the combination of higher efficiency at higher power and increased operating frequencies may facilitate operating the lamp at higher power levels for shorter intervals of time, facilitating dimming.

At higher operating frequencies it may be possible to avoid using ferromagnetic materials for the coupler core and instead use a material that has a magnetic permeability essentially the same as that of free space, and an electrical conductivity of zero, or close to zero. One type of material that satisfies these conditions is plastic, but one skilled in the art will appreciate other materials that meet this characteristic and suitable for this application. Couplers wound on rods or tubes that satisfy the stated conditions are typically referred to as ‘air-core couplers’ or ‘air-core coils’. An air-core coil may also be fabricated without the use of any rod-like or tubular coil form if the wire is sufficiently stiff or if the wire is supported by an external structure. The use of an air-core coil may enable the printing of the coupler windings on the air side of the re-entrant cavity, enable the removal of the reentrant cavity and placement of the air coil directly in the bulb with electrical feedthroughs to the outside, and the like.

The use of an air-core coil rather than a coil wound on a ferromagnetic core may result in cost and weight savings. Additionally, an air-core coil may be less temperature sensitive than a coil that uses a ferrite core. Magnetic materials have a temperature limitation above which their magnetic characteristics are severely affected. Conversion to an air-core coil eliminates the need to control the core temperature to preserve magnetic performance as a design limitation.

In some embodiments, the fundamental frequency may be selected from one of a set of frequencies, known as the industrial, scientific and medical (ISM) radio bands. Devices emitting electromagnetic radiation in these bands are not subject to the typical FCC restrictions on the strength of such emissions, so these bands are especially useful for devices, such as induction lamps, that use radio frequency energy for non-communication purposes.

In one embodiment, the fundamental operating frequency is 27.12 MHz. There is an ISM band centered at 27.12 MHz and having a bandwidth of 326 KHz allowing for greater operating latitude for both the primary operating frequency and side band emissions. FIG. 29 shows a DC-to-AC inverter circuit designed for operation at approximately 27 MHz. The increased latitude at this operating frequency may allow for the frequency to be generated using a less precise and less costly ceramic resonator, or similar device, rather than a quartz crystal. In one embodiment, the fundamental operating frequency is 40.7 MHz. There is an ISM band centered at 40.680 MHz and having a bandwidth of 40 KHz. In one embodiment, the fundamental operating frequency is approximately 13.6 MHz. There is an ISM band centered at 13.560 MHz and having a bandwidth of 14 KHz. In one embodiment, the fundamental operating frequency is approximately 6.8 MHz. There is an ISM band centered at 6.8 MHz and having a bandwidth of 30 KHz. In one embodiment, the fundamental operating frequency is between 2.5 and 3 MHz.

Ballasts that employ the basic AC-to-DC converter stage described herein, consisting of a full wave bridge rectifier and an energy storage capacitor, will usually draw current from the AC power line only near the peak of the AC voltage waveform. This leads to what is known as “low power factor” and “high total harmonic distortion.” Low power factor and high harmonic distortion are not serious issues for many consumer applications, but would create problems in commercial and industrial applications. Low power factor is also undesirable in consumer applications if the ballast is to be used on a circuit controlled by a TRIAC-based incandescent lamp dimmer.

The TRIACs used in conventional lamp dimmers expect the lamp load to draw current during all parts of the power line cycle. This current is used by the dimmer to charge the TRIAC firing circuits at the start of each power line half-cycle, and to maintain the TRIAC in the “on” state until the voltage drops to zero before changing polarity every half-cycle. A conventional low power factor circuit draws current only during a small part of the power line cycle; the part of the cycle when the power line voltage is near its peak value. TRIAC-based dimmers therefore do not work properly when driving ordinary low power factor ballasts.

Ballasts can be modified in at least the following five ways to make them compatible with TRIAC-based dimmers:

In embodiments, a special “active power factor correction” circuit can be added to the ballast. This is typically a separate power conversion stage such as a buck or boost converter that is designed to draw current from the AC power line over essentially the full AC cycle. The current drawn generally has a sinusoidal wave shape.

In embodiments, a “charge pump” circuit can be used to feed some of the energy from the output of the ballast back to the input, and use this energy to draw small amounts of current from the AC power line at the frequency of the high frequency inverter. Charge pump circuits can create a sinusoidal input current, like that produced by an active power factor correction stage, or they can draw smaller currents that are not high enough to create a sinusoidal current input but are still high enough to provide TRIAC trigger and holding current.

In embodiments, the single energy storage capacitor may be replaced with two or more energy storage capacitors connected in such a way that they charge in series but discharge in parallel. These so-called “passive valley fill” circuits will draw current over a greater portion of the AC cycle than a single power line frequency energy storage capacitor, leading to improved power factor and lower total harmonic distortion.

In embodiments, the energy storage capacitor can be removed completely, or separated from the output of the full wave bridge rectifier, so that the circuit naturally draws power over most of the AC cycle. This type of circuit may benefit from the addition of an auxiliary power supply that can provide enough power keep the lamp operating when the power line voltage drops to a low value as it changes polarity twice each cycle.

In embodiments, an impedance element, such as a resistor or capacitor can be connected to the output of the full wave bridge so that some current is drawn from the AC power line over the full AC cycle, even when the remainder of the ballast is using power stored in the energy storage capacitor and not drawing current from the AC power line. Further, the impedance element can be switched in and out of the circuit at a frequency higher than the power line frequency, or have its value adjusted by a control circuit so as to provide the required current load, while minimizing power loss.

In embodiments, a dimming device load control facility may enable the induction RF fluorescent lamp to provide for electrical loads required for the proper operation of an external control dimming device, the dimming device load control facility controlling an electrical load or impedance element that may be switched in and out of connectivity within the electronic ballast to provide a load for the external dimming device. The electrical load or impedance element is switched out of the circuit during on-time intervals of the external dimming device and switched into the circuit during off-time intervals of the external dimming device.

The dimming device load control facility may comprise processor-based management and control facilities, such as with a microcontroller, a digital processor, embedded processor, microprocessor, digital logic, and the like. The methods and systems described herein may be deployed in part or in whole through a machine that executes computer software, program codes, and/or instructions on a processor, and implemented as a method on the machine, as a system or apparatus as part of or in relation to the machine, or as a computer program product embodied in a computer readable medium executing on one or more of the machines. The processor may be at least in part implemented in conjunction with or in communication with a server, client, network infrastructure (e.g. the Internet), mobile computing platform, stationary computing platform, cellular network infrastructure and associated mobile devices (e.g. cellular phone), or other computing platform. The integrated circuit electronics may comprise a single package with a combination of analog and digital integrated control circuits.

The microcontroller or the like may determine the operational state of the induction RF lamp, running, start-up, or off, by monitoring operational characteristics of the induction RF lamp including transformer voltage, coupler voltage, coupler current, and the like. Transformations may be done on the collected operational characteristics and they may be compared against set parameters, previously stored values of the operational characteristics, ratios of current to previous values and the like.

In embodiments, the dimming device load control facility may detect the presence of an external dimming control device and switch in a load. In embodiments, the dimming device load control facility may detect the type of external dimming control device such as leading-edge type, trailing-edge type, smart type, and the like, and automatically adjust the control of the switched electrical load based on the detected device type. Control adjustments may comprise where in the AC power cycle the induction load is switched in and out of the electrical circuit. The switching of electrical load based on the detected external dimming control device type may be optimized to improve induction RF lamp performance such as reducing flicker in the lamp, reducing power consumption and noise and the like.

Burner

The burner is constructed of a transparent or translucent vitreous material formed in the shape of the desired light-emitting element. For the type of induction lamp described herein, an open cylindrical cavity, often referred to as a reentrant cavity, penetrates one side of the outer jacket of the burner. The inner surface of the burner and the surface on the partial vacuum side of the reentrant cavity are typically coated with at least one material, called ‘phosphor’ in the lamp industry, that converts ultraviolet energy into visible light. The coating may Aluminum Oxide, Al₂O₃, phosphor, mixed Aluminum Oxide, Al₂O₃ and phosphor, and the like. The partial vacuum surface of the reentrant cavity may first be coated with a reflective material, such as magnesium oxide (MgO) or the like, before the phosphor is applied. Such reflective material reduces the amount of light lost to the air side of the reentrant cavity and thus increases the burner efficacy.

The partial vacuum surfaces of the burner may be optionally coated with an initial thin, transparent or translucent barrier layer, commonly Alon (fine particulate Aluminum Oxide, Al₂O₃), or “pre-coat” which may reduce chemical interactions between the phosphor and the glass, the mercury (Hg) and the glass, and may help adhesion of the phosphor to the glass. The burner is evacuated and then filled with a rare gas, such as Neon, Argon or Krypton generally at a pressure of 13 Pascal to 250 Pascal. The outer bulb and reentrant cavity are generally made from glass, such as soda lime glass or borosilicate glass.

The performance of the burner is a function of the dimensions of the outer bulb used to form the burner, the dimensions of the reentrant cavity, the type of rare gas fill, the pressure of the rare gas fill, the pressure of the mercury vapor (which, as is described below, is a function of the amalgam composition and the amalgam temperature), the quality of the phosphor, the thickness and particle size of the phosphor coating, the process used to burn the binder out of the phosphor, and the quality of the exhaust process.

In addition to the rare gas described above, a small amount of mercury is added to the burner before it is sealed. Often times, in order to extend the ambient temperature range of operation of an induction lamp, a mercury amalgam is used instead of pure mercury. While this allows the lamp to operate at elevated ambient temperatures (for example in hot fixtures), at room temperatures or lower ambient temperatures it may take a longer time to obtain the full light output due to the very low mercury pressure before the lamp warms up to operating temperature. This is referred to as ‘run-up time’, and a long run-up time (e.g., 30 seconds or longer) is not desired, especially in residential applications. The mercury is commonly combined with other metals, such as bismuth, tin, indium or lead to form an amalgam. For example, the main amalgam composition may range from 10% by weight of indium to 98% by weight of indium. The composition of the main mercury amalgam will influence the mercury vapor pressure during steady state operation; therefore, the choice of composition of mercury amalgam may be influenced by a desire to optimize the mercury vapor pressure and corresponding light output at the steady state operating temperatures of the burner. The mercury or mercury amalgam is typically placed in at least two locations in the burner.

In embodiments, an amalgam may be placed in the sealed end of the exhaust tube. An amalgam may be placed in the bulbous envelope such as above the re-entrant cavity, at the base of the bulb, or the like. An amalgam may be encapsulated in borosilicate glass, other vitreous material such as soft glass, fused silica, aluminosilicate glass, ceramics, and the like, a metal tube, or other material during the preparation and evacuation of the burner cavity to minimize the loss of mercury during manufacturing. The encapsulation may be breached using a laser, mechanical perforation, radio-frequency heating system or other device after the burner cavity has been sealed enabling mercury vaporized during subsequent heating to diffuse into the burner cavity. In other embodiments, the encapsulation may be formed with a tiny hole to permit mercury vapor to escape and inserted into the bulb just prior to final gas processing and sealing of the bulbous envelope. This may be done after the baking of the envelope so that no mercury is lost during the baking process.

As the size of the lamp decreases, it may be more difficult to position the amalgam in the evacuation tube below the coupler. In embodiments, the amalgam may be placed in a capsule positioned inside the bulbous envelope above the re-entrant cavity 3020. A capsule 3002 (FIG. 30A-30B) holding the amalgam 3004 may be held above the re-entrant cavity using a bent wire mount 3008. The bent wire mount 3008 may include a single capsule attachment wire 3010 having two ends with a first end attached to the capsule. The capsule attachment 3018 may be a mechanical attachment such as the single capsule attachment wire 3010 twisting around the capsule 3002, the capsule attachment wire 3010 may be embedded into the capsule 3002 during capsule formation, and the like. The second end of the capsule attachment wire 3010 may be attached to a capsule support structure 3014 using a mechanical attachment 3012 such as a weld, twisted wires, and the like. The capsule support structure 3014 may comprise at least two wires or two ends of the same wire extending below the capsule, bowing outward. The bowed wires are compressed together and inserted into the evacuation tube 3022 in the center of the re-entrant cavity. The bowed wires of the bent wire mount 3008 then press against the interior surface of the evacuation tube 3022, holding the capsule in place due to friction. However, there are disadvantages to the bent wire mount as there are few lines of contact between the bent wire mount 3008 and the interior surface of the evacuation tube. Under certain circumstances such as during shipping, the lamp may be jostled. This may cause the capsule 3002 containing the amalgam 3004 to shift, touching the inner surface of the bulbous envelope. This may result in scratching or removal of a portion of the phosphor that coats the inner surface of the bulbous envelope. The scratches may be visually unappealing and result in uneven illumination. Alternately, the movement of the lamp may result in the bent wire mount 3008, and the capsule 3002 comprising the main amalgam 3004, slipping further into the re-entrant cavity. This would position the amalgam 3004 closer to or inside the power coupler, subjecting the amalgam 3004 to increased temperatures, potentially resulting in an unfavorable change in the mercury vapor pressure. In some embodiments, two bent wire mounts oriented perpendicular to one another may be used to hold the capsule in place. In some embodiments, a single wire may provide the functionality of the capsule attachment wire 3010 and the capsule support structure 3014.

In embodiments, an alternate way of positioning the capsule 3002 containing the amalgam 3004 above the re-entrant cavity may include the use of a helix mount 3108 (FIG. 31A-B). The helix mount 3108 may include a single wire tightly twisted in the middle or two wires with the one end of each the wires tightly twisted together. The tightly twisted portion 3102 may be attached to the capsule and the two ends of the wire may be shaped into turns with the wire ends turning in opposite directions. The turns may be entwined together to form a shape resembling a double helix 3104. The helix mount 3108 may be attached to the capsule 3002 using a mechanical attachment, a portion of the tightly twisted portion 3102 may be embedded into the capsule glass 3002, and the like

An alternate configuration of the helix mount 3208 may include a single capsule attachment wire 3210 having two ends with a first end attached to the capsule. The second end of the capsule attachment wire 3210 may be attached to a capsule support structure, in this case the double helix 3104, using a mechanical attachment 3212 such as a weld, twisted wires, and the like. The double helix 3104 may include at least two wires or two ends of the same wire shaped into turns with the wires or wire ends turning in opposite directions. The turns may be entwined together to form a shape resembling a double helix 3104. There may also be a tightly twisted section 3102 near the mechanical attachment 3212.

The capsule 3002 may be positioned above the re-entrant cavity using a helix mount 31083208 with the double helix 3104 portion inserted into the evacuation tube 3022 of the re-entrant cavity 3020, the entwined turns providing multiple points of contact between the wires of the double helix 3104 mount and the interior surface of the evacuation tube, resulting in increased friction with the surface of the evacuation tube relative to the bent wire mount 3008, and thus, less movement of the capsule 3002. The wires may be made of metals that do not react with mercury, whose coefficients of thermal expansion are similar to the material of the bulbous envelope, evacuation tube and re-entrant cavity, and which retain flexibility and springiness across a range of temperatures. The wires may be molybdenum, tungsten, nickel, stainless steel and similar materials. The wires may be approximately 0.375 mm in diameter, enabling the wires to be embedded into the borosilicate glass of a preformed capsule using heat. The wires may be embedded into the borosilicate glass of the capsule prior to the insertion of the capsule containing the amalgam through evacuation tube and into the lamp envelope.

In a non-limiting example, testing has revealed that a capsule held in place with a single bent wire mount 3008 made of molybdenum wire exhibited a pull-out force or strength of 0.3 Newtons to dislodge the mount and capsule. A double bent wire mount made of molybdenum wire exhibited a pull-out force or strength of 0.7 Newtons. Whereas, a capsule held in place with a helix mount made of molybdenum wire and having approximately 2.0 turns exhibited a pull-out force or strength of 2.4 Newtons and a helix mount made of molybdenum wire and having approximately 2.5 turns exhibited a pull-out force or strength of 4.0 Newtons. A helix mount made of stainless steel wire and having approximately 2.5 turns exhibited a pull-out force or strength of 3.7 Newtons. A helix mount made of molybdenum wire and having more than 3.0 turns was found to be stiff, making it difficult to insert into the evacuation tube, and as a result the force required to insert the mount may result in spring elongation and deformation of the turns of the mount due to frictional forces. The wire used in all of the above examples was approximately 0.375 mm in diameter. Thinner wire such as wire that is approximately 0.1 mm in diameter may not provide an adequate pull-out force or strength. Thicker wire, such as wire that is approximately 0.5 mm in diameter, may result in increased transfer of thermal energy from the interior of the coupler core to the amalgam capsule, possibly resulting in an increase in amalgam temperature.

Flag

In embodiments, one or more flags, comprising a material with which mercury may create an amalgam, are positioned in the main part of the burner cavity. After an initial run-time, the burner is turned off and some of the mercury vapor released into the burner cavity during operation will settle on the inside surfaces of the burner cavity, migrate back to a main or secondary initial amalgam, settle on one or more flags and the like. The vapor that condenses on the one or more flags may create an amalgam, while the remaining mercury in the burner will either migrate back to a main or secondary amalgam or eventually find its way to one or more flags, further enriching the flag amalgam with mercury. The mercury in the flag amalgam may be released more quickly during subsequent lamp starts than the mercury in the main amalgam, thereby shortening the run-up time considerably. The discharge created by the induced electric field will ideally heat the flag, releasing the amalgamated mercury on the flag before the temperature of the main amalgam, located below the power coupler, or a secondary amalgam located above the coupler is sufficiently heated to vaporize the mercury at that location.

In embodiments, the flag may be attached to the bulb in several different ways, such as shown in FIGS. 22A and 22B. FIG. 22A shows a flag 2202 with a pin 2204 that is embedded into the cavity wall 2208. FIG. 22B shows a flag 2210 with a pin 2212 that is mechanically placed in the lamp without the need for an additional seal.

However, placement of the flag in the main part of the burner cavity alone still may not provide satisfactory performance for residential applications, where consumer studies have indicated that the end user typically requires at least 70-80% of the final light output in less than one second. This can be described as a relative light output (RLO) of 70-80%. The present disclosure describes a new flag design, with size, configuration, and materials combination so as to yield a significantly shorter time frame with respect to a goal of a 70-80% RLO (as compared to the final steady state value). In embodiments, the flag configuration may comprise the number of flags, radial distance of the flag or flags from the surface of the reentrant cavity, vertical position of the flag or flags along the length of the reentrant cavity, orientation of the flag or flags relative to the reentrant cavity, the length, width and thickness of the flag, the material used to fabricate the flag, the shape of the reentrant cavity, and the like. The flag configuration may be optimized to provide short run-up time while maintaining high efficiency during steady state operation.

In embodiments, the induction lamp described herein may provide for a rapid build-up of luminosity during the starting of the lamp. The flag may be positioned within the lamp envelope so as to maximize lamp maintenance. The flag may be positioned inside the lamp envelope so as to enable a minimum cost and practical placement for manufacturing of the lamp with high-speed equipment. The induction lamp described herein may provide for a very large number of multiple lamp starts, such as many tens of thousands, without suffering poor maintenance or drop in RLO at a specific time after start.

The induction power coupler creates a time-varying magnetic field that, in turn, creates a first time-varying electric field within the burner envelope. The time-varying magnetic field is aligned parallel to the cavity axis and the first component of the time-varying electric field is aligned perpendicular to the time-varying magnetic field and encircles that field. Electrical breakdown of the burner gas occurs in the presence of the established electric field and a time varying current is established in the direction of the electric field. Within this field may be placed a first metallic object, flag, which is substantially flat along a plane and having a normal perpendicular to the plane. The orientation of the flag relative to the cavity axis, and thus the flag's orientation relative to the time-varying electric field and current, determines the effective surface area of the flag perpendicular to the time-varying induced electric field. The flag may be positioned so the normal of the surface of the flag is directed radially, toward the coupler (or the plane of the flag is substantially “parallel” to the cavity axis). In this position, the normal of the surface of the flag is oriented at an angle of 0 degrees relative to the normal of the surface of the re-entrant cavity. Alternately the flag may be positioned so that the normal of the surface of the flag is directed in the azimuthal direction (or “perpendicular” to the re-entrant cavity axis). In this position, the normal of the surface of the flag is oriented at an angle of 90 degrees relative to the normal of the surface of the re-entrant cavity. In other embodiments, the flag may be oriented at some angle between these orientations. FIG. 22C shows these two different orientations for placing the flag with respect to the axis of the cavity, with the flag 2214 mounted “perpendicular” to the vertical axis of the cavity with the normal of the surface of the flag oriented at an angle of 90 degrees relative to the normal of the surface of the re-entrant cavity and the flag 2218 mounted “parallel” to the cavity axis (wherein the structure of the flag 2218 is not seen in the view because the normal of the flag is in the plane of the drawing sheet). The flag 2218 is mounted such that the normal of the surface of the flag is oriented at an angle of 0 degrees relative to the normal of the surface of the re-entrant cavity. Note also that the illustrated representation of the structure of the flags 22142218 are one of a plurality of possible structural configurations, and are not meant to be limiting in any way.

In preferred embodiments, the flag is oriented such that the angle of the normal of the surface of the flag relative to the normal of the surface of the re-entrant cavity approaches 90 degrees. In embodiments, the flag 2214, with its “perpendicular” orientation to the cavity axis and larger surface area perpendicular to the time-varying electric field, may enable increased interaction with the current driven by the time-varying induced electric field. This in turn may facilitate faster heating of the flag element and faster introduction of mercury vapor into the burner envelope, thus reducing warm-up time.

In some embodiments, the first flag 2220 material may be a solid piece of metal. In other embodiments, a metal mesh may be used for the first flag 2220 to provide multiple sharp edges that may act as field enhancement points. In embodiments, a mesh material may also be used in place of a solid material to reduce the mass of the first flag 2220, which may lead to more rapid warm-up. The mesh may comprise a cut metal that has been expanded, woven wires, punched metal and the like. The metal of flag, mesh or solid, may comprise steel, stainless steel, nickel, titanium, molybdenum, tantalum and the like. The metal of the first flag 2220 may be plated with Indium or the like to facilitate the formation of an amalgam with the mercury. The first flag 2220 may be substantially flat along a plane. In embodiments, the surface area of the flag with respect to the time-varying electric field may be increased by folding the flag material into two or more sections, such as aligned parallel to one another in close proximity or constrained along the plane. An example of this is shown in FIG. 22D. Folded flag 2220A is positioned with a perpendicular orientation to the cavity axis and, in contrast, folded flag 2220B is positioned with a parallel orientation to the cavity axis.

In embodiments, the one or more first flags 2220 may be positioned between 0 and 12 mm radially outward from the surface of the re-entrant cavity and between the re-entrant cavity and the outer wall of the envelope. In preferred embodiments, the one or more first flags 2220 may be positioned between 2 and 5 mm from the re-entrant cavity and between the re-entrant cavity and the outer wall of the envelope. The position of the flag within the main part of the burner cavity affects the energy being absorbed by the flag structure. For instance, the magnitude of the time-varying electric field falls off with distance from the axis of the coupler. The distance of the flag to the coupler also correlates to breakdown voltage. The relationship of breakdown voltage to the product of gas pressure and distance between the electrodes appears to be similar to a Paschen-like curve, an example of which is shown in FIG. 23. At a single pressure, a Paschen-like curve describing breakdown voltage is a function of distance alone for a mono-component gas, such as a rare gas. At a single distance, the Paschen-like curve describing breakdown voltage is a function of pressure alone. When both the distance and pressure are changed, a Paschen-like curve describing breakdown voltage is a function of the product of the distance and the pressure. It may be desirable to co-optimize the distance of the flag from the coupler together with the pressure within the burner envelope in such a way that the breakdown voltage is low at both start-up, when the gas in the burner is predominantly rare gas, and during steady state operation, when the pressure within the burner is slightly higher and due to the small admixture of mercury vapor pressure. In general, the shape of the Paschen-like curve remains similar as mercury is added to the rare gas filling, but the magnitude of breakdown voltage is lowered and the minimum shifts to a different value of the product of gas pressure and distance.

If the rare gas used is Argon rather than a gas such as Krypton, the starting voltage will be much lower due to the well known Penning effect, in which the ionization of the mercury is greatly enhanced by collisions with Argon metastable atoms. The Penning effect will dominate in many Mercury-Argon discharges and may be the main driver for flag placement in burners with Mercury and Argon, where it may be preferable to place the flag in the center of the burner space, such as mid-way between the reentrant cavity and the outer wall of the bulb.

In a preferred embodiment where the rare gas is a mix of mercury and krypton, the breakdown voltage may approach a minimum at an optimum product of distance and gas pressure. As the product of flag location (distance from the re-entrant cavity) and gas pressure goes below optimum, voltage needed to initiate the arc in the plasma increases dramatically. Alternately, as the product of radial distance of the flag from the coupler and gas pressure increases beyond the optimum, the voltage required to initiate the arc in the plasma beings to increase slowly. At room temperature start-up, the mercury pressure inside the burner cavity will be lower than at steady-state operation. The pressure inside the burner cavity begins to rise as the mercury amalgam on the flag is heated and mercury released. Subsequently, the amalgam positioned below the coupler may be heated and additional mercury vapor released into the burner cavity. At the lower initial pressure, it may be desirable to position the flag at an increased distance from the coupler to achieve a low breakdown voltage near a Paschen-like minimum. However, a flag located at the greater distance from the power coupler may have reduced interaction with the time-varying current, leading to slow heating of the flag and the release of the mercury from the flag amalgam which would translate into a slower warm-up. It is therefore advantageous to consider the inclusion of multiple flags, each of which is tasked with a definite purpose.

Positioning one or more flags at various radial distances from the centerline of the cavity axis enables different flag-field interactions. In one embodiment, illustrated in FIG. 22E, one or more flags are positioned within the burner cavity. A set of one or more first flags 2220A, 2220B may be positioned in proximity to the coupler such that interaction with the electric field driven current is facilitated and release of mercury from the amalgam contained in this flag is optimized. Positioning this set of one or more first flags 2220, in this illustration the folded flag 2220A or 2220B, closer to the coupler may increase the amount of heating by a combination of the electric field and the discharge due to positioning it close to the radial current maximum, which may result in more rapid heating of the flag and release of mercury into the re-entrant cavity

One or more starting aid flags 2224 may be located at a distance from the centerline of the cavity axis to facilitate optimization of the product of pressure and distance at the reduced pressure that may be present at lamp start-up. For instance, this starting aid flag 2224 may be used to facilitate the initiation of the plasma by being positioned such that the breakdown voltage for the working gas mixture described by a Paschen-like curve is reduced relative to the location of the first flag 2214. This starting aid flag 2224 may be positioned between the first flag 2214 and the outer wall of the burner envelope. This starting aid flag 2224 may provide a small, pointed surface area such as a wire, the edge of a foil or sheet, or the like to facilitate electric breakdown of the working gas. This starting aid flag 2224 may be mounted to the surface of the re-entrant cavity. This starting aid flag 2224 may be attached to the mount for another flag 2214 such as with a spot weld 2228 or the like. This starting aid flag 2224 may be comprised of a conductive metal that is not reactive with mercury such as steel, stainless steel, nickel, molybdenum, tantalum or the like. It is preferable that the starting aid flag 2224 not comprise materials suitable for amalgam formation, such as indium and the like. FIG. 22E is meant to be illustrative and is not limiting with respect to the presence, type, position or orientation of the second flag.

In some embodiments, the flag material may be a solid piece of metal. In other embodiments, a metal mesh may be used for the flag to provide multiple sharp edges that may act as field enhancement points. When high voltage is applied at starting, the flag charges like one electrode of a capacitor and the field is enhanced by the sharp edges, providing enhanced voltage needed for breakdown. In embodiments, a mesh material may also be used in place of a solid material to reduce the mass of the flag, which may lead to more rapid warm-up. The mesh may comprise a cut metal that has been expanded, woven wires, punched metal and the like. The metal of flag, mesh or solid, may comprise steel, stainless steel, nickel, titanium, molybdenum, tantalum and the like.

In embodiments, it is desired to optimize mercury vapor pressure in the burner envelope. For example, the optimum mercury vapor pressure may be approximately 0.9 Pascals. As the mercury vapor pressure falls below the optimal value, the generation of UV radiation is reduced, resulting in a lower light output. As the mercury vapor pressure exceeds the optimum value the generated UV radiation is reabsorbed by the mercury vapor due to the higher mercury density. The subsequent non-radiative process prevents this diverted excitation from producing UV excitation of the phosphor resulting in reduced light output of the lamp.

In embodiments, there may be two or more amalgams of mercury positioned at various locations within the lamp to provide vaporized mercury during operation of the lamp. The amalgams may have different compositions and may contribute to lamp operation in different ways. One amalgam is referred to herein as the “main” amalgam. The purpose of the main amalgam is to sustain the optimal mercury concentration throughout the life of the lamp. The main amalgam typically has an amount of mercury content that, if it were all vaporized at once, would result in a mercury vapor pressure well above the optimum. However, the main amalgam is typically positioned to regulate the speed at which the amalgam is heated and the maximum temperature reached by the amalgam, so the main amalgam warms up slowly and acts as a regulator for mercury pressure during operation, and the maximum temperature is regulated such that the mercury is not fully vaporized during normal operation. Note that another reason for the main amalgam having more mercury than necessary for the operation of the lamp is that over time there is some loss of mercury from the main amalgam due to interactions with the phosphor, glass, and the like, so selection of the initial amount of mercury in the main amalgam factors into the life of the lamp and the performance of the lamp over its lifetime.

Mercury amalgam may also be provided on one or more structures within the lamp envelope called flags. These amalgams contain a small amount of mercury relative to the amount of mercury desired for optimum mercury vapor pressure. The intent of the mercury on the one or more flags is to provide a small amount of mercury into the vapor phase more quickly than the main amalgam could provide, in order to increase the rate at which light is developed in the lamp and thus decrease the time the lamp takes to reach maximum illumination.

Upon initial start-up of a lamp, the overall temperature of the lamp increases due to power dissipation in the plasma and, on a longer time scale, thermal diffusion from the lamp electronics. At start-up, the temperature distribution is non-uniform throughout the lamp, with temperatures being higher in proximity to the power coupler and ballast electronics. The main amalgam may be positioned in the evacuation tube such that it heats slowly and reaches a relatively low maximum temperature. The amalgams on the one or more flags may be positioned in the burner envelope in such a way as to heat more quickly than the main amalgam. Positioning of the flag in different locations within the envelope may result in different rates of mercury vaporization from the flag. For instance, an amalgam on a flag positioned near the power coupler may heat more quickly due to its proximity to the power coupler, which acts as a source of heat when power is applied. As the amalgam heats up, the mercury vapor pressure increases to the point all of the mercury on that flag is vaporized. The mercury vapor will migrate around the burner envelope. This temperature point is dependent on the composition of the amalgam. The amalgam on the flag is designed to capture a limited amount of mercury and release essentially all of it during the start-up phase. The total amount of mercury released during the start-up phase will produce a vapor pressure less than what will finally be achieved when the main amalgam reaches its operating temperature.

After the lamp is shut-down, it will cool, and the mercury vapor will condense and settle on the walls of the burner, condense onto the flags disposed within the lamp, and/or migrate back to the main amalgam site, and the like. To optimize lamp performance, it may be desirable to specify different material compositions for the main amalgam and any flags so as to optimize the relative mercury vapor pressures and facilitate the condensation of the mercury onto the flags rather than migration back to the main amalgam site. This may be done by selecting a main amalgam composition such that it has a higher vapor pressure at room temperature than the second or other amalgam that is initially formed on a flag. For instance, in one embodiment a flag may be formed of indium with the resulting condensed amalgam being one of indium and mercury, and with the corresponding main amalgam being one of bismuth, indium and mercury. In another embodiment, the main amalgam may be one of bismuth, tin, indium, and mercury.

In embodiments, the flag substrate may be made of a material that does not form an amalgam with mercury, where this material is then coated with another material that will form an amalgam with mercury, such as indium or the like. In embodiments, this approach will provide an additional source of mercury, more available for vaporization, such as above and beyond what is provided in the amalgam. In embodiments, the flag may be the only source of mercury in the lamp. Flag substrate materials may include metals such as steel, iron, nickel, stainless steel, tantalum, tungsten, molybdenum, and the like. Flag substrate materials may include non-metallic substrates, such as quartz, glass, polymers, such as polyimide, or ceramics made from sintered aluminum oxide (Al₃O₂) and the like, where the ceramic substrate may be plated using an electroless coating with a material, such as tungsten or the like, prior to plating with a material that will form an amalgam with mercury, such as indium and the like.

While indium is very effective in absorbing and releasing mercury within the lamp, it sputters readily, can easily be ejected from the flag, and re-deposit on the inside of the lamp. Once this occurs, the indium is no longer in the correct position to act as a secondary source of mercury and assist startup. Additionally, the indium would then be deposited on the inside of the lamp, which tends to cause discoloration and reduce lumen output. Since the indium is saturated with atmospheric mercury, the bulb would then be coated with not only indium, but also elemental mercury and mercurous or mercuric oxides. Therefore, keeping the indium intact on the flag, preventing it from sputtering or ejected from its original position and deposited on the inside of the lamp, is highly desired.

While the exterior of the induction bulb is maintained at approximately 75 C, the internal lamp temperature is much higher and can often exceed the melting point of indium, which melts at 156.6 C. Since sputtering rate is dependent on density and surface energy, and since indium expands as a liquid, the sputtering rate of liquid indium would be higher than solid indium. Therefore, keeping indium from melting during normal lamp operation is also highly desired.

For electrodeless lamps, the flag is heated by the radio frequency (RF) flux, generated by the electrical ballast. However, the flag temperature can also be controlled by the flag's mass and specific heat, which is defined by the rate of heat flow through per unit area, per unit temperature gradient in the direction perpendicular to the area. The temperature gradient, for a given RF flux, can be reduced by reducing the path length, flag thickness or mass. Therefore, a thinner flag having a lower mass, comprised of a material with a higher specific heat, would heat faster, evolve adsorbed mercury faster, and cause the lamp to light up faster. Additionally, the material and shape of the flag can determine the rate which heat is removed from the flag. For instance, by using a wire connected to the flag, with different thermal conductivity, the flag may be cooled to make it last longer (e.g., using a molybdenum vs. a stainless-steel support wire). Where this support wire runs and where it is attached may also change the thermal profile of the flag. Another means for cooling the flag may include placing a glass bead on the wire to dissipate heat (e.g., in the cool area), thus making the flag cooler.

One common method of altering the specific heat of a flag is to form an alloy or a mixture of more than one metal. Indium is capable of alloying with many metals, however few have the same property of amalgamating with mercury. Such a property, of absorbing mercury, is common with indium, which allows the metal to absorb and release atmospheric mercury and function as a secondary mercury source. Gold, for example, also has the property of amalgamating with mercury, being second only to indium for that purpose.

Furthermore, alloys of gold and indium have much higher melting points, therefore indium-gold alloy coated flags will not melt during lamp operation. This means that the sputtering rate is reduced, not only because the alloy remains a solid throughout lamp operation, but also because the sputtering rate of gold is much less than indium. Since the sputtering rate is reduced, the indium is not ejected from the flag during normal operation and thus will remain on the flag longer and retain its function longer as a secondary mercury source. Furthermore, the lumen maintenance will be greater, since the reduced sputtering will reduce the deposition of indium or mercury on the bulb and the lamp will start up more rapidly.

No gold will diffuse into an adjacent coating of indium, however interstitial indium will diffuse into the gold and produce an alloy of AuIn or AuIn₂ even at room temperature. Both alloys can be produced when indium and gold are present, such as when there is at least 35% indium and 65% gold (weight-to-weight). Since there is also a minimum amount of indium required to absorb the atmospheric mercury in the lamp, and since some of the indium is converted into an alloy, a small excess of indium may be required to replace the indium that has now been converted into a gold-indium alloy.

In a non-limiting embodiment, a foil or mesh flag may be first coated with gold, followed by a coating of indium, such that the gold to indium weight-weight ratio is 15 to 85 percent; but not to exceed 10 to 90 percent. Methods of depositing the indium and gold include DC sputtering, electroless or electrolytic plating methods, and the like. In an example, a 4 gram per square meter coating weight of the gold may be first applied, followed by a 22 gram per square meter coating weight of the indium, such as by utilizing a method of electrolytic plating.

As the indium diffuses into the gold sub-layer, AuIn or AuIn₂ alloys are formed, which produce an intermediary coating between the gold and indium. These alloys of AuIn or AuIn₂ also act as an adhesion layer for the indium and maintains a smooth, high surface area indium coating, whether solid or liquid. The high surface area is key for optimum adsorption of mercury by the indium coated flag. In order to maintain sufficient indium on the flag, additional indium must be added to compensate for the AuIn or AuIn₂ alloy produced. Therefore, a minimum ratio of indium to gold is required for rapid start performance, otherwise, the AuIn or AuIn₂ would consume all of the indium on the flag.

The flag may consist of various materials, including metals (e.g., tin, molybdenum, nickel, stainless steel), metal oxides (e.g., silicon dioxide (quartz) or aluminum oxide), and the like. Flags which will be fabricated from metal oxides, such as quartz, may first need to be coated with an electrically conductive coating, such as nickel, before plating the gold or indium. Ideally, the flag material should have as little mass as possible, such as for example, a weight less than 200 mg, 100 mg, and the like. In embodiments, the flag structure may consist of a woven-wire mesh (e.g., having wires approximately 20-25 microns in diameter), foil (e.g., having a thickness of approximately 10-15 microns thick), perforated foil, and the like. The thermal conductivity of the flag material should also be low, such as where the flag material is fabricated from stainless steel mesh, foil, thin quartz or polyimide sheets.

Although alloys of gold and indium have been used herein to describe an improved flag material, it will be appreciated by one skilled in the art that other alloy combinations with similar properties may also utilized, such as using tin (Sn) or nickel (Ni) to form an alloy with indium. Tin or nickel, as well as titanium (Ti), platinum (Pt), and the like, could also function as supporting flag materials.

Referring to FIG. 44, there is a preferred range of mercury pressure 4402 at which the lamp emits an optimum level of light output. If the mercury vapor pressure is below the preferred range 4404, too little UV energy may be generated within the lamp and the luminous output of the lamp decreases. If the mercury vapor pressure is above the preferred range 4408, more UV energy is generated, however, there may also be an increase in radiation trapping where the generated photon is absorbed by the mercury before it is able to interact with the phosphors, resulting in a decrease in luminous output of the lamp. The particular amalgam composition that results in mercury vapor pressure being in the preferred range 4402 during steady state operation of the lamp varies with a plurality of factors such as amalgam composition, operating temperature of the lamp and the amalgam, power consumption of the lamp, lamp geometry, color temperature of visible light generated from conversion of UV energy by phosphors, and the like.

In an embodiment, a test may be performed to facilitate selection of amalgam composition that will result in the mercury vapor pressure being in the preferred range 4402 and optimize luminous output of the lamp. Referring to FIG. 45, the amalgam testing system 4500 generally includes a device to measure total light output of the lamp as a function of time such as an integrating sphere 4502, a way to rapidly cool a portion of the lamp such as a cooling spray applicator 4504 and cooling spray 4508.

Referring to FIG. 46, the amalgam composition selection process 4600 describes a series of steps to evaluate the performance of a given amalgam composition and compare results of different amalgam compositions (step 4610). In some lamps, measurements of amalgam temperature may be used to evaluate different amalgam compositions. However, in some embodiments, the amalgam location is positioned inside the lamp envelope making thermal measurements difficult. The amalgam performance measurement process 4612 generally includes positioning the lamp within an integrating sphere 4502 or other device for measuring the total light output of the lamp as a function of time (step 4602). Typically, the lamp is run for approximately an hour, achieving steady state operation (step 4604), a cooling spray such as compressed gas, cooled compressed gas, and the like, is applied to a small portion of the lamp (step 4608). The application of the cooling spray (step 4608) acts as thermal perturbation to the lamp, rapidly cooling a portion of the lamp and condensing mercury vapor while leaving the main amalgam uncooled at steady state operating temperature.

In a non-limiting example, shown in the lamp output measurements 4700 of FIG. 47, a lamp operating with a preferred range of mercury pressure 4402 would exhibit an optimum light output 4702 having a high level steady state light output 4710 and decreasing monotonically with cooling of the bulb 4714 after the cooling spray is applied 4712. The light output decreases as the mercury pressure decreases due to the mercury vapor condensing on the cooling bulb. If the mercury vapor pressure is below the preferred range 4404 the lamp will exhibit a light output 4708 with steady state light output 4710 reduced relative to that achieved at an optimum mercury pressure 4402 and decreasing monotonically with cooling of the bulb 4714 after the cooling spray is applied 4712. If the mercury pressure is above the preferred range 4408 the lamp will exhibit a light output 4704 with steady state light output 4710 reduced relative to that achieved at an optimum mercury pressure 4402. Note that in this case, after the cooling spray is applied 4712, the light output may increase for a period of time as the mercury pressure decreases due to the mercury condensing on the cooling bulb, moving into the preferred range of mercury pressure 4402. But after further cooling of the bulb, the light output will drop as the mercury pressure continues to drop to below the preferred range 4404.

As part of the amalgam composition selection process 4600 measurements may be made for a series of lamps having different amalgam compositions. Based on the lamp output measurements 4700 it may be possible to determine whether the amalgam should be adjusted so as to change the mercury vapor pressure at steady state. If the light output curve exhibits an increase when the cooling spray is applied, the amalgam should be altered to achieve a lower level of mercury vapor pressure, such as by decreasing the total amount of mercury in the amalgam, increasing the other metallic components of the amalgam such as indium, bismuth, tin and the like. If the light output curve does not exhibit an increase when the cooling spray is applied, it is possible that the mercury vapor pressure is too low. A sample with a higher mercury vapor pressure may be used as a discriminant between optimum mercury vapor pressure and suboptimal (too low) mercury vapor pressure. A sample with a higher mercury vapor pressure may be produced such as by increasing the amount of mercury in the amalgam, decreasing the other metallic components in the amalgam, and the like. If the sample with the higher mercury vapor pressure exhibits higher luminous output at steady state, the amalgam composition is adjusted in that direction.

In an illustrative example, a set of lamps was built having different amalgam compositions. Each lamp was A19 in geometry, operating at approximately 14.4 Watts and having phosphors that resulted in visible light with a color temperature of approximately 2700K. The operating temperature of the lamp was in the range of 65 C-90 C and the amalgam, positioned above the re-entrant cavity was approximately in the range of 100 C to 125 C. The three amalgam compositions shown in Table 1 were tested resulting in light output measurement curves similar to those shown in shown in FIG. 47.

TABLE 1
Composition of Various Amalgams
	% Indium	% Mercury	% Other Metals
Amalgam Composition A	33	3.5	63.5
Amalgam Composition B	37.5	3.3	59.2
Amalgam Composition C	36.1	3.3	60.6

The light output from the lamp with amalgam composition A exhibited a characteristic shape 4704 representative of a lamp operating above the preferred range of mercury vapor pressure 4408. The light output from the lamp with amalgam composition B exhibited a characteristic shape 4708 representative of a lamp operating below the preferred range of mercury vapor pressure 4404. The light output from the lamp with amalgam composition C exhibited a characteristic shape 4702 representative of a lamp operating in the preferred range of mercury vapor pressure 4402. Additional amalgam compositions were tested and a range of amalgam compositions resulting in mercury vapor pressure in the optimum range 4402 identified. An A19 lamp, operating at approximately 14.4 Watts, having a color temperature of approximately 2700K and running about 65 C to 90 C with the amalgam deployed in an ampoule at the top of the evacuation tube, has an optimum amalgam composition of approximately 35.38%-36.82% Indium by weight, Mercury of 3.27%-3.33% by weight and other metals ranging from 59.39%-61.81% by weight.

Coupler

The coupler generates, the AC magnetic field that provides, through magnetic induction, the electric field that drives the discharge. In addition, the voltage across the coupler is used to start the discharge through capacitive coupling.

The AC magnetic field created by the coupler changes in both intensity and polarity at a high frequency, generally between 50 kHz and 50 GHz. In the preferred embodiment, the coupler is a multi-turn coil of electrically conductive wire that is connected to output of the inverter. The AC current produced by the inverter flows through the coil and creates an AC magnetic field at the frequency of the inverter. The coil can optionally be wound on a “soft” magnetic material such as ferrite or iron powder that is chosen for its beneficial properties at the frequency of the AC current. The ferrite material can be easily formed into numerous shapes; such as a torus or a rod, or other shapes, depending upon the design of the burner, when in the so-called “green state,” before it is fired to form a hard ceramic. Iron powder can be pressed into similar shapes. In the preferred embodiment, the coupler is formed from a coil of copper wire wound on a rod-like ferrite tube. The ferrite is tubular in that it has a hole along the axis to allow passage of the exhaust tube of the burner. For the preferred embodiment, the operating frequency is 1 to 10 MHz.

In another embodiment, the frequency is increased to the 10 MHz to 50 MHz range and the ferrite tube is removed and optionally replaced by a rod or tube made from a material that has a magnetic permeability essentially the same as that of free space, and an electrical conductivity of zero, or close to zero. One type of material that satisfies these conditions is plastic. Couplers wound on rods or tubes that satisfy the stated conditions are called ‘air-core couplers’ or ‘air-core coils’. An air-core coil can also be fabricated without the use of any rod-like or tubular coil form if the wire is sufficiently stiff or if the wire is supported by an external structure. The use of an air-core coil may enable the printing of the coupler windings on the air side of the re-entrant, or removal of the reentrant and placement the air coil directly in the bulb with electrical feedthroughs to the outside, and the like.

The burner is designed to provide a discharge path that encircles the time-varying magnetic field. As is known from Faraday's Law of Induction, a voltage will be induced in any closed path that encircles a time varying magnetic field. That voltage will have the same frequency as the frequency of time-varying magnetic field. This is the voltage that drives the induction-coupled discharge.

The ferrite material is chosen for low power loss at the frequency of the AC current and at the magnetic flux density and temperature where it is designed to operate.

The number of turns on the coupler is chosen to provide a good impedance match for the inverter when connected through the matching network. It is generally desirable to have a coupler composed of at least 5 turns of wire to ensure efficient coupling to the discharge, while it is also desirable to have the turns form a single layer winding on the ferrite, if used, or form a single layer coil if an air core is used. These practical considerations set desirable lower and upper limits on the number of turns of the coil.

Management and Control

In embodiments, the induction lamp may include processor-based management and control facilities, such as with a microcontroller, a digital processor, analog processing, embedded processor, microprocessor, digital logic, and the like, and implemented in an integrated circuit, an application-specific integrated circuit, and the like. The methods and systems described herein may be deployed in part or in whole through a machine that executes computer software, program codes, and/or instructions on a processor, and implemented as a method on the machine, as a system or apparatus as part of or in relation to the machine, or as a computer program product embodied in a computer readable medium executing on one or more of the machines. The processor may be at least in part implemented in conjunction with or in communication with a server, client, network infrastructure (e.g. the Internet, WiFi network, local network of lamp nodes), mobile computing platform, stationary computing platform, cellular network infrastructure and associated mobile devices (e.g. cellular phone), or other computing platform.

Management and control facilities may receive inputs from external switches on the induction lamp, from IR/RF remote control inputs from remote controllers, from a networked interface (e.g. a wireless network interface such as WiFi, wireless LAN, Bluetooth, HomeRF, cellular, mesh, and the like, or wired network interface such as through existing home wiring e.g. IEEE Powerline), and the like. For instance, an embedded controller may receive settings via switches mounted on the lower portion of the induction lamp, such as for color control, lumen output control, power savings modes, dimmer compatibility, and the like. In an example, there may be a switch setting to enable-disable dimming functionality, such as to provide a power savings as the result of disabling a dimming functionality. In another instance, a remote control or networked control interface may be used to control functions of the induction lamp, such as power management, light characteristics settings, dimming control, on-off control, networked control settings, timer functions, and the like. In an example, the induction lamp may be controlled through an RF remote control of the known art where the induction lamp includes an RF receiver interfaced to an embedded processor, where the RF remote controller controls lighting levels, such as on-off and dimming control. In another instance, a first induction lamp may be commanded directly by a remote controller (e.g. RF/IR remote control, networked controller, an embedded controller in conjunction with another networked lamp node with a network of lamps), where the first induction lamp also acts as a repeater by sending the command on to at least one of a plurality of other induction lamps. In an example, a plurality of induction lamps may be controlled with a single remote-control command, where induction lamps within range of the remote controller respond to the direct command, and where induction lamps not within direct range of the remote controller (such as because of distance, obstructions, and the like) are commanded by commands being repeated by induction lamps that had received the command (such as by any induction lamp repeating the command when received). In embodiments, the processor-based management and control facilities may provide for a control function, such as associated with the operation of the electronic ballast, comprising at least one of control of a startup condition, control of an operating mode, control of a dimming function, control of a color temperature, control of a user interface, control of a remote-control interface, control of a network interface, control of a thermal management function, and the like.

Management and control facilities may include a processor-based algorithm that provides at least partial autonomous management and control from parameters determined internal to the induction lamp, such as for color control, lumen output control, power management, and the like. For instance, lumen output control may be implemented at least in part by a processor-based algorithm where inputs to the processor may include feedback signals from the inverter output, and where inputs from the processor include control signals as an input to the inverter. In this way, the processor-based algorithm may at least in part replace analog feedback functionality, such as to provide greater control of the lumen output through internal algorithms utilizing data table mappings of inverter output current vs. luminous output, and the like. The algorithm may also accept control via commands to the induction lamp, such as from a switch setting, a remote-control input, a command received from another induction lamp, and the like.

In embodiments, the processor-based management and control facilities may enable a more compact layout of the ballast electronics. For instance, the electronic ballast may be laid out utilizing a control processor in place of discrete components to aid in the ability of the induction RF fluorescent lamp to fit within the exterior dimensions similar to that of an ordinary incandescent bulb, as discussed herein. In an example, the electronic ballast may be contained within a tapering portion of the induction RF fluorescent lamp that tapers from a bulbous vitreous portion to the screw base such that the bulbous vitreous portion, the tapering portion, and the screw base taken together provide exterior dimensions similar to that of an ordinary incandescent bulb (e.g. at least one of a member of an A-series, BR-series, PAR-series lamps).

Thermal

In embodiments, the induction lamp may manage thermal dissipation within the structure, such as through a dynamic power management facility utilizing a processor-based control algorithm, through a closed-loop thermal control system, through thermal-mechanical structures, and the like. Indicators of thermal dissipation, such as temperature, current, and the like, may be monitored and adjusted to maintain a balance of power dissipated within the induction lamp such as to meet predetermined thermal requirements, including for maximizing the life of components within the induction lamp, maintaining safe levels of power dissipation for components and/or the system, maximizing energy efficiency of the system, adjusting system parameters for changes in the thermal profile of the system over a dimming range, and the like. In an example, power dissipation across a dimming range may create varying power dissipation in the system, and the dynamic power management facility may adjust power being dissipated by the ballast in order to maintain a maximum power requirement. In another example, maximum power dissipation for the system or components of the system may be maintained in order to maintain a life requirement for the system or components, such as for temperature sensitive components.

Thermal management facilities may be utilized to help manage the thermal environment of the induction lamp. For example, electrical components may often be mounted in such a way that the electrical components are located against a printed circuit board (PCB). Positioning electrical components, such as FETs, in this way may result in reduced mechanical stress on the electrical component and on the electrical/mechanical connections between the electrical component and the PCB. Also, the electrical component may be lying in such a position that a heat pad on the electrical component, if present, is touching the PCB. In this way, the PCB may act as a heat spreader for the electrical component. The PCB may be designed in such a way that thermal management features such as metal pads (e.g. made of copper), thermal vias to move heat to the other side of the board, radiation structures (e.g., vanes or fins), and the like, are incorporated into the PCB during manufacturing of the board, to enhance the spreading of heat away from the electrical component through the thermal facility of the PCB.

Referring to FIG. 35, in embodiments, one or more of the lamp's electrical components 3504, such as the field effect transistors (FETs) may be mounted upright relative to the PCB 3502 to conserve space and achieve a desired form factor. However, when the one or more electrical components 3504 is mounted in an upright orientation relative to the PCB 3502, the PCB 3502 is less effective as a way to dissipate a portion of the heat generated by the one or more electrical components 3504. Thus, it may be desirable to provide other ways to dissipate the heat generated by the one or more electrical components 3504. In embodiments, the one or more vertically mounted electrical components 3504 may be mounted along the edge of the PCB 3502. Referring to FIGS. 36-37, a heat spreader 3602 may be used to dissipate the majority of the heat generated by the one or more vertically mounted electrical components 3504. The heat spreader 3602 may be shaped such that its perimeter approximates the perimeter of the PCB 3502 and has standoffs 3604 such that the heat spreader 3602 may be positioned above the PCB 3502, allowing thermal contact to be made between the heat spreader 3602 and a heat pad 3702 located on the back of the one or more vertically mounted electrical component 3504. The heat spreader 3602 may include cutouts 3608 of different forms and shapes such as holes, squares, reduced heights, and the like, as needed to allow for the passage of wires and the like and to provide clearance relative to other components. The heat spreader 3602 may be a closed shape or open with a slit or break 3610. The embodiment with a slit may present manufacturability advantages. The heat spreader 3602 may be circular or may have partially flattened or linear sections 3704 to facilitate good thermal contact between the heat spreader 3602 and a thermal pad 3702 on the one or more vertically mounted electrical components 3504. The heat spreader 3602 may be made of a thermally conductive material such as copper, aluminum, and the like. Although a single heat spreader 3602 has been described, there may be more than one heat spreader 3602 with smaller heat spreaders associated with individual electrical components 3504 contemplated.

Referring to FIGS. 38-39, there may be a clip 3802 to facilitate thermal contact 3702 between the heat spreader 3602 and the at least one vertically mounted electrical component 3504 while minimizing mechanical stress on the at least one vertically mounted electrical component 3504. The clip 3802 may be solid or have cut-outs to facilitate air circulation and reduce weight. In some cases, such as where there is a heat spreader associated with an individual electrical component 3504, the heat spreader may be attached directly to the electrical component using a thermal conductive material such as solder or the like. In some embodiments, the heat spreader, rather than being a stand alone band around the PCB, may be a copper or aluminum strip along the inside of the lamp housing.

In some embodiments, electrical components 3504 and heat spreader 3602 may be totally or partially embedded in a potting compound. While the use of a potting compound is known in the art, the selection of potting material to have increased thermal conductivity is not common. The use of a potting compound having increased thermal conductivity may provide for improved dissipation of the heat generated by the electrical components 3504 during lamp operation. The PCB 3502, electrical components 3504 and heat spreader 3602 may be potted together or various combinations of electrical components 3504 and heat spreaders 3602 may be potted individually.

In a non-limiting experiment, a series of lamps were built where two of the electrical components 3504, FETs, were mounted in an upright position and placed in thermal contact with a heat spreader 3602. The electrical components 3504 and heat spreader 3602 were then potted and measurements were made of the temperature of various electrical components. As seen in Table 2, increasing the thermal conductivity (k) for the potting compound resulted in a reduction in the temperature of the various electrical components. Reducing the operating temperature for these electrical components results in increased component life.

TABLE 2
Component Temperatures for Potting Materials with
Various Thermal Conductivities
	Material	Potting	Potting	Potting
	Thermal Conductivity	Material 1	Material 2	Material 3
	(W/mK)	(k = 0.7)	(k = 1)	(k = 1.44)
	Component	Temperature (° C.)
	Coupler	208	207	188
	Toroid	124	116	111
	RF Board	115	107	103
	Heat Sink	107	102	97
	Capacitor	92	90	85

Electrical and Mechanical Connection

In embodiments, the electrical-mechanical connection of the induction lamp may be standard, such as the standard for incandescent lamps in general lighting, including an Edison screw in candelabra, intermediate, standard or mogul sizes, or double contact bayonet base, or other standards for lamp bases included in ANSI standard C81.67 and IEC standard 60061-1 for common commercial lamps. This mechanical commonality enables the induction lamp to be used as a replacement for incandescent bulbs. The induction lamp may operate at AC mains compatible with any of the global standards, such as 120V 60 Hz, 240V 50 Hz, and the like. In embodiments, the induction lamp may be alterable to be compatible with a plurality of standard AC mains standards, such as through an external switch setting, through an automatic voltage and/or frequency sensing, and the like, where automatic sensing may be enabled through any analog or digital means known to the art.

Dimming: Improved Dimming Circuits

Phase controlled TRIAC dimmers are commonly used for dimming incandescent lamps. A TRIAC is a bidirectional gate controlled switch that may be incorporated in a wall dimmer. A typical dimmer circuit with an incandescent lamp is shown in FIG. 2, where the TRIAC turns “on” every half of the AC period. The turn “on” angle is determined by the position of the dimmer potentiometer and can vary in range from 0 to 180 degrees in the AC period. Typically, the lighting dimmer is combined with a wall switch. An incandescent lamp is an ideal load for a TRIAC. It provides a sufficient latching and holding current for a stable turn “on” state. The TRIAC returns to its “off” state when the current drops below a specific “holding” current. This typically occurs slightly before the AC voltage zero crossing. But wall dimmers do not operate properly with most normal single stage ballasts.

Besides holding and trigger currents, the TRIAC should be provided with latching current, that is a sufficient turn “on” current lasting at least 20-30 usec for latching the TRIAC's internal structure in a stable “on” state. A ballast circuit may have an RC series circuit connected across the ballast AC terminals to accommodate the TRIAC. But steady power losses in the resistor could be significant. Other references have similar principles of operation, such as based on drawing high frequency power from the bridge rectifier.

Other previous work discloses a TRIAC dimmable electrodeless lamp without an electrolytic storage capacitor. In this case the ballast inverter input current is actually a holding current of the TRIAC and is high enough to accommodate any dimmer. The lamp ballast is built as self-oscillating inverter operating at 2.5 MHz. An example block diagram of a dimmable ballast is shown in FIG. 3. It comprises an EMI filter F connected in series with AC terminals, a Bridge Rectifier providing high ripple DC voltage to power a DC-to-AC resonant inverter, and a Resonant Tank loaded preferably by inductively coupled Lamp. The ballast inverter is preferably self-oscillating inverter operating in high frequency range (2.5-3.0 MHz). A TRIAC dimmer is connected in front of the ballast providing phase-cut control of the input AC voltage.

Related art teaches operation from a rectified AC line live voltage that varies from almost zero volts to about 160-170V peak. A self-oscillating inverter may start at some instant DC bus voltage, such as between 80V and 160V, but it will stop oscillating at lower voltage (usually in a range between 20V and 30V). FIG. 4 illustrates a related art dimming method where Vm 402 is a voltage waveform after the TRIAC dimmer. This voltage is rectified and applied to the input of the inverter. Without an electrolytic storage capacitor, the ballast inverter (not shown in FIG. 4) stops its operation during the TRIAC “off” intervals. Accordingly, the electrical discharge in the lamp burner stops and starts, such as illustrated in lamp current I_LAMP 404 in FIG. 4.

Other related art discloses a TRIAC dimmed electronic ballast that utilizes a charge pump concept for an inductively coupled lamp. This method requires injecting RF power from the inverter into the full wave bridge rectifier used to convert the 60 Hz AC power into DC power. Accordingly, the 60 Hz bridge rectifier must be constructed using diodes that are rated for the full power line voltage and ballast input current, and are also fast enough to switch at the inverter frequency without excessive power loss.

Therefore, there may be embodiments for operating high frequency electrodeless lamps powered from TRIAC-based dimmers that reduce or eliminate the capacitor(s).

In accordance with an exemplary and non-limiting embodiment, a method for dimming a gas discharge lamp with a TRIAC-based wall dimmer is provided. The method may provide uninterruptible operation of the lamp and the ballast during TRIAC dimming. The method may include powering the ballast without an electrolytic smoothing capacitor, directly from the rectified AC voltage that is chopped by the TRIAC dimmer, and supporting lamp operation during the off time of the TRIAC, such as with a smoothing electrolytic capacitor-less D.C. bus. Implementation of the method may include additional features comprising charging a small low voltage capacitor from the DC bus via a DC-to-DC step down current limiting converter during the TRIAC “on” intervals and discharging this capacitor directly to the DC bus during TRIAC “off” intervals, for maintaining uninterruptable current in the gas discharge lamp.

In another aspect, the invention may feature a DC current charge circuit for charging a low voltage capacitor. In one of disclosure embodiments the charger may be built as charge pump connected to the output of the ballast resonant inverter.

In the other aspect, for dimming of inductively coupled lamps, the invention may feature a secondary series resonant tank for stepping down the DC bus voltage for charging a low voltage capacitor. The secondary resonant tank may be coupled to the switching transistors of the ballast resonant inverter.

FIG. 5 shows block-circuit diagram of an electronic ballast connected to a TRIAC dimmer 502. The dimmer 502 may be for instance, a wall dimmer aimed for controlling incandescent lamps. The electronic ballast may feature a front-end power supply without a traditional smoothing capacitor, such as with a smoothing electrolytic capacitor-less D.C. bus. It may comprise an EMI filter 504, a Bridge Rectifier 508, a high frequency Inverter 512 (e.g. a 2.5 MHz inverter), and resonant load that includes Matching Network 514 and electrodeless Lamp 518. In accordance with exemplary and non-limiting embodiments, the high frequency inverter may be selected to operate at a very wide frequency range such as tens of KHz to many hundreds of MHz. The Matching Network 514 may utilize a circuit having resonant inductor LR 520 and resonant capacitor CR 522 with the Lamp 518 connected in parallel with the resonant capacitor CR 522. An auxiliary low voltage (40-50V) DC power supply 510 may be connected to the DC bus 524 of the inverter via a backup diode D 528 for filling in rectified voltage valleys. The power supply 510 may be built as a DC-to-DC step down converter powered from the DC bus 524. The auxiliary DC power supply 510 may comprise a small low voltage storage capacitor (which may be electrolytic or tantalum type) for maintaining uninterruptable low power lamp operation during the TRIAC “off” time intervals. The R-C network 530 may be connected across the diode D 528 for providing latching current pulse of very short duration (20-40 usec) to the TRIAC after its triggering. By having a low voltage power supply 510 (40-50V or even lower), a wider dimming range may be achieved.

In FIG. 6, dimming operation of the lamp and ballast of FIG. 5 is illustrated by showing wave forms of the DC bus voltage V_BUS 602, Lamp voltage V_L 604, Lamp current I_L 608, and auxiliary power supply current I_AUX 610. In comparison with the prior art method demonstrated in FIG. 3, the lamp current continues during the TRIAC “off” intervals, so that the ballast and the lamp do not need to restart. To keep the Lamp “on” at minimum current only 15-20% of nominal lamp power may be needed. This power may be obtained from an external or internal DC source.

In accordance with exemplary and non-limiting embodiments a method for a dimming gas discharge lamp powered by an electronic ballast with a front-end power supply without an electrolytic smoothing capacitor is provided. Said method may feature uninterruptible lamp operation and comprises steps of charging a low voltage storage capacitor during the TRIAC “on” time intervals and discharging said low voltage storage capacitor to the DC bus during the TRIAC “off” time intervals. Since the low voltage storage capacitor for supporting lamp operation must store only a small amount of energy, its overall size may be substantially less than the size of a storage capacitor in the prior art dimmed ballasts with boosting voltage charge pumps. Since auxiliary voltage V_AUX may not exceed 50V, a miniature tantalum capacitor may be used in the ballast.

In accordance with exemplary and non-limiting embodiments an electronic ballast is provided without an electrolytic DC bus smoothing capacitor. FIG. 7 illustrates a block-circuit diagram in an embodiment of the disclosure, preferably for RF electronic ballasts. It may comprise a ballast connected to a TRIAC dimmer (not shown). The ballast front-end power supply may comprise an EMI filter 702 and a bridge rectifier 704. There may not be a traditional electrolytic capacitor connected in parallel to the output of the bridge rectifier 704. A self-oscillating inverter 708 may be built with a half bridge topology but other relevant inverter topologies may also be used. The inverter 708 may comprise a pair of series MOSFET switching transistors Q1710 and Q2712, connected across DC bus 714, a capacitive divider with capacitors C1718 and C2720 across the DC bus 714, parallel loaded matching network 722 having a first series resonant inductor LR1724 and a first resonant capacitor CR1728. Inductively coupled Lamp 730 may be connected in parallel to the first resonant capacitor CR1728. The combination of the matching network and the inductance of the lamp coupler forms a first resonant circuit. Transistors Q1710 and Q2712 may be driven by a drive circuit 732 coupled to the inverter 708 via a positive feedback 734 circuit (not shown), for self-excitation of the inverter 708.

In accordance with exemplary and non-limiting embodiments, FIG. 7 shows the auxiliary power supply combined with the inverter power stages, comprising the transistors Q1710 and Q2712. The inverter 708 may include a low voltage storage capacitor C_ST 738 having a positive terminal connected to DC bus 714 via a backup diode D 750 and a negative terminal connected to DC bus negative terminal. The inverter 708 may also feature a second, series loaded, current limiting resonant tank 740 comprising a second resonant inductor LR2742 and a second resonant capacitor CR2744. A secondary high frequency rectifier having diodes D1752 and D2754 may be connected in series with the indictor LR2742 and capacitor CR2744. Rectified current charges the storage capacitor C_ST 738. A ceramic bypass capacitor (not shown) may be connected in parallel to the storage capacitor C_ST 738 for RF application. The power of the second resonant circuit may be much less than the first one, so that a tiny Schottky diode array, for instance, BAS70-04 may be used for 752 and 754 in the secondary rectifier circuit. An RC-network 748 may be connected across the diode 750 for conditioning the external TRIAC dimmer. In the ballast of FIG. 7, the storage capacitor C_ST 738 may have much less energy storage than a traditional DC bus high voltage capacitor, where its rated voltage may be about 50V. The low voltage storage capacitor C_ST 738 may have much smaller dimensions than the traditional high voltage DC bus capacitor in prior art ballasts.

In accordance with exemplary and non-limiting embodiments, FIG. 8 demonstrates another low-cost configuration. This embodiment differs from that presented in FIG. 7 by the way in which the storage capacitor C_ST 738 is charged. In the inverter 708 of FIG. 8 C_ST 738 is charged by a charge pump from the inverter output. A series capacitor Cp 802 is connected between the inverter high voltage terminal LH 808 and the diode configuration of D1752 and D2754. Charge current is determined by value of capacitor Cp 802. A bypass capacitor C_B 804 may be connected across the storage capacitor C_ST 738.

Comparatively, the arrangement in FIG. 8 may provide faster low voltage capacitor C_ST 738 charging during lamp starting. But it may slow down the starting process of an electrodeless lamp by taking power from the lamp and returning said power to the inverter input. Also, this power feedback may cause system stability problems during steady-state system operation because of the negative incremental impedance of the lamp.

The additional component LR2742 in FIG. 7 may provide full decoupling from resonant load and the lamp. It may provide reliable starting and high efficiency due to the step-down feature of the series load connection. To help guarantee Zero Voltage Switching (ZVS), the second resonant tank should operate in inductive mode, such as when ωLR2>1/ωCR2. In an example, for a 20 W electrodeless lamp operating at 2.75 MHz, the values of secondary resonant circuit components may be the following: LR2=150 uH, CR2=18 pF; Schottky diode array BAS70-04, electrolytic capacitor C_ST=22 uF, 50V. A bypass capacitor 0.1 uF is connected across the electrolytic capacitor C_ST.

The lamp may be dimmed because of a variation of the RMS voltage applied to the lamp, with a condition that the minimum required lamp current is sustained. Some minimum DC bus voltage should be provided to ensure continuous ballast and lamp operation. During TRIAC dimming both the TRIAC formed voltage and the DC backup voltage may vary and cause lamp dimming. The lower the minimum backup voltage the wider the dimming range. This minimum voltage depends on many factors determined by the lamp and ballast or combination of both characteristics. For a 2.5 MHz electrodeless lamp the minimum operation voltage for continuation of burning may be about 38-40V at 20° C. ambient temperature.

FIG. 9 shows actual oscillograms taken from operation of a 20 W, 2.75 MHz electrodeless lamp using a ballast with the preferred embodiment, when powered with a TRIAC dimmer. Ch2904 shows the TRIAC dimmer output voltage, Ch1902 shows lamp voltage, and Ch3908 shows lamp current. The backup DC voltage is about 45V. As can be seen the lamp and ballast operate continuously with the TRIAC dimmer. In this example, the lamp is dimmed to 60%.

At low bus voltage, lamp voltage (Ch1) is increased, since the gas discharge is characterized by negative impedance. Inductively coupled lamps are distinguished by a significant leakage inductance. That is why lamp voltage increases correspondingly with lamp current (Ch3).

Dimming: Burst Mode Dimming

Burst mode dimming is a method to control the power delivered to the burner, and the light generated by the burner that uses periodic interruptions of the high frequency signal delivered to the coupler from the ballast.

One way to control the power delivered to the burner and hence control the light output of the burner, is to turn the high frequency current delivered by the ballast to the coupler, I_C, on and off on a periodic basis at a rate that is much lower than the frequency of the high frequency current itself. That is, if the high frequency current has a frequency of f_O (e.g., in the 1 MHz to 50 MHz region) and the rate of the periodic signal is f_M, then f_M would be much lower than f_O. In embodiments, f_M may be less than one-tenth of f_O in order to better ensure that the resulting dimming would not produce perceptible flickering.

In embodiments, the dimming signal may be synchronized to the lamp current waveform, so that lamp drive current is always provided in full half-cycles of the lamp operating frequency. This is intended to reduce the generation of RF energy at frequencies other than the lamp operating frequency, since such energy could interfere with RF communication devices operating at frequencies other than the operating frequency of the lamp. Further, the drive current I_C may be a sinusoidal, or near sinusoidal, drive current.

The time duration of each On period and each Off period of I_C will be less than 1/f_M, and the sum of the time duration of the On period and the time duration of the Off period will equal 1/f_M. Since f_M is much lower than f₀, each On period of I_C will ideally have more than 10 cycles of I_C.

In some embodiments, it may be desirable that the Off period time of I_C be shorter than the time required for the electron density of the discharge to substantially decrease. For the exemplar induction coupled lamp, this time is believed to be about 1 msec.

In other embodiments, it may be desirable that the Off period time of I_C be longer than the time required for the electron density of the discharge to substantially decrease. For the exemplar induction coupled lamp, this time is believed to be about 1 msec.

In some embodiments, it may be desirable that f_M be higher than 20 kHz, so that the circuits used to generate this signal do not create audible noise, while in other embodiments it may be desirable that f_M be lower than 20 kHz so that the Off period time duration of I_C can be longer than the time required for the electron density to substantially decrease.

For example, if f_M is set to 25 kHz the Off time will always be less than 0.04 msec. In addition, if f_M is set to 25 kHz, and the On time is set to 1% of the time rate of the modulation frequency, 1/25 kHz, the On time will be 0.4 μsec, and this time period will contain 10 cycles of I_C when f₀ is 25 MHz. In this manner, periodic bursts of current at a frequency of f₀ and controllable duration can be applied to the coil that is driving the lamp or discharge.

This power control method may be used to reduce the power delivered to the lamp when less light is required and less power consumption is desired. This is known in the art as dimming.

The dimming function can be controlled by a circuit that senses the firing angle of a TRIAC-based phase cut dimmer installed in the power supply for the lamp, or it may be controlled by a control means mounted on the lamp itself, or by radio waves or by infrared control, or any other suitable means.

The power control method can also be used to provide accurate operation of the lamp without the use of precision components in the high frequency oscillator. The circuit could be designed to produce somewhat more than the rated power of the lamp, and then the burst mode power control could be used to reduce the power to the rated value.

The power control could also be used to provide shorter run-up times for mercury-based lamps. When used in this manner, the circuit providing I_C would be designed to produce 20% to 50% more current than necessary for steady state operation. When the lamp is cold and the mercury vapor pressure is low, the extra current would provide more light and facilitate faster heating of the mercury, which would, in turn, provide a faster rise in mercury vapor pressure from its value at room temperature toward the optimum mercury vapor pressure, which occurs at temperatures higher than 20° C. As the lamp warms up to its normal operating temperature, the power control would reduce the power gradually to its normal value. The lamp would not overheat when operated at higher than normal power to implement this feature because the higher power would be applied only when the lamp is at a temperature lower than its normal operating temperature.

TRIAC Holding and Trigger Current: Pass-Through Current

It is desirable for all types of lighting, especially screw-in light bulbs, to be compatible with TRIAC-based phase cut dimmers due to the low cost and ubiquitous presence of these dimmers in lighting installations. These dimmers are wired in series with the AC line voltage and the lighting load. Accordingly, any current drawn by the dimmer circuit needs to pass through the load. In particular, these dimmers include a timing circuit in which the applied line voltage charges a capacitor through a variable resistor. Each half-cycle of the line frequency, the capacitor is charged up to a threshold voltage at which a semiconductor break-over device (typically a 32 volt DIAC), conducts a pulse of trigger current into the gate terminal of the TRIAC to put the TRIAC into a conductive state.

A resistive load like an incandescent light bulb naturally conducts the current required by the timing circuit for triggering the TRIAC into the on-state. In contrast, electronic circuits, such as used with fluorescent lamps, may not conduct current at low input line voltages. Typically, they include an energy storage capacitor to hold up the supply voltage for the load continuously throughout the line cycle. In the case of a fluorescent ballast, this energy storage capacitor typically supplies an inverter circuit that converts the DC voltage on the storage capacitor to an AC current for powering the fluorescent lamp. When the instantaneous line voltage is low, the rectifier or other circuit that charges the energy storage capacitance will not draw current from the line. Even without an energy storage capacitor, there will be a minimum voltage required for the inverter or other electronic circuit to operate.

In addition to the timing circuit of the dimmer, some dimmers may contain one or more indicator LED's or other electronics that require the load to pass current for proper operation.

A resistor placed across the input of the electronic ballast might draw the required pass-through current prior to the dimmer TRIAC switching to the on-state; however, the full line voltage would be applied to this resistor while the TRIAC is on, therefore dissipating too much power and generating too much heat for this to be a practical solution.

In embodiments, a circuit may be provided with a resistor load that is switched relative to at least one threshold level. For instance, the resistor load may be switched on when the applied line voltage falls below a relatively low threshold, and off when the applied line voltage exceeds the threshold. In this way, a load is presented to the TRIAC to provide the required pass-through current when the voltage is low (e.g., when the ballast is in a state that does not provide a sufficient path for such current), and removes the resistor load when the voltage is high, thus eliminating the power dissipated in the resistor at a time when the resistor is not needed to provide pass-through current. In another instance, there may be multiple threshold levels, such as to provide hysteresis for rising verses falling voltage levels. In embodiments, rather than completely switching out the resistor during the entire time the line voltage is high, the resistor may be switched in and out as a pulsed current load, thus providing a way to modulate the load resistor's effect. For example, the resistor may be switched (e.g., by way of a transistor circuit) at a 100% duty cycle when the line voltage is below the set threshold, and at a reduced duty cycle, such as a 10% duty cycle, when the line voltage is above the set threshold.

Referring to FIG. 10, an example circuit is illustrated where the threshold is set for 10 volts. V1 represents the input line voltage presented by the dimmer. Q1 and Q2 form a Darlington transistor pair for switching load resistor R1, and these transistors must be rated about 200V or higher for a 120 VAC line. Resistor R2 provides base drive to Q2. With a net current gain (beta) value of at least 500, Q2 will, for example conduct approximately 15 mA (pass-through/trigger current) with 6V on the input line. When the input voltage exceeds approximately 10V, resistors R3 and R4, bias Q3 into the active region where it conducts enough current to cut off the base drive to Q1/Q2.

The value of R1 is selected here such that, even if the maximum of 10 volts were applied to the circuit continuously, power dissipation would be only about ¼ watt. Normally, the power dissipation would be much less than this because the series resistance in the dimmer is normally 10 kiliohms or larger, resulting in less than 3.5% of the line voltage appearing across the pass-through circuit, and once the TRIAC is triggered, the applied voltage would exceed the 10 volt threshold, thereby blocking current flow in the load resistor R1.

Besides varying resistor values and resulting threshold voltages, other embodiments of this invention, may replace the combination of Q1/Q2 with a switch such as a MOSFET (with a Zener diode to protect its gate), or under some conditions, a single bipolar transistor may provide sufficient gain. Q3 can also be implemented by some other switch or its function may be incorporated into an integrated circuit.

This discrete circuit can operate with very low voltages across the ballast input and begin to draw current when the supply voltage exceeds a small threshold voltage, approximately 1.2V in the embodiment of FIG. 10. This feature allows the circuit to operate when the TRIAC is off, giving smoother operation during startup and at very low dimmer settings where the TRIAC does not turn on. An LED on the dimmer, for example, could still be lit by this pass-through circuit at such low dimmer settings.

The load resistor will not be connected all the time, either continuously or pulsed, while the resistor in this invention will be disconnected when the voltage is higher than the set point.

Other Dimming, TRIAC Holding, and Trigger Current Circuits:

Other circuits and/or components associated with dimming, TRIAC holding, and trigger current may provide benefits, such as a charge pump, a voltage boost, an AC load capacitance, a constant current load, a circuit for limiting electrolytic capacitor current with a current source, a circuit for providing frequency dimming, a circuit for providing amplitude dimming, a shutdown circuit, and the like. For instance, the induction lamp may be dimmed through a plurality of methods, such in embodiments described herein. Each method has advantages and disadvantages that depend on the embodiments implemented in the induction lamp, such as load characteristics, ballast circuit characteristics, and the like. For example, as an alternative to other dimming methods described herein, shifting the frequency operating point at which the electric ballast operates may reduce the load current, and thus dim the induction lamp. This is referred to as frequency dimming. Another embodiment includes a method of reducing the power level provided to the load, such as by reducing the supply voltage, which then reduces the load current, thus providing a dimming of the induction lamp. This is referred to as amplitude dimming. Selection of a dimming method may also include combinations of these methods, as well as with the various methods described herein.

EMI

The issue of electromagnetic interference (EMI) inflicted by any industrial and consumer product utilizing RF power is the subject of strict domestic and international regulations. According to these regulations, the EMI level emanating from RF light sources must not exceed some threshold value that may interfere with operation of surrounding electronic devices, communication, remote control gadgets, medical equipment and life supporting electronics. The permitted EMI level for consumer lighting devices is relaxed at frequencies from 2.51 MHz to 3.0 MHz, but the increase in allowable EMI is limited and EMI still has to be addressed to comply with the regulations.

EMI generated by the electronics, such as from the ballast of the induction lamp, may be mitigated through the use of shielding around the electronics, such as with a solid or mesh conductor surrounding the electronics (e.g. the ballast electronics), around the electronics compartment, around the interface between the power coupler and the electronics, and the like, thus creating a Faraday cage around the electronics and keeping electromagnetic radiation from emanating from the electronics portion of the induction lamp. A very thin conductive foil may be selected because of resulting savings in weight and/or cost of materials. This thin foil may be in contact with or supported by a non-conductive material to help maintain dimensional integrity of the thin conductive foil. A mesh may be selected rather than a solid because of the resulting savings in weight and/or cost of materials, increased flexibility in accommodating the packaging of the electronics, and the like. When a mesh is selected, any holes of the mesh are made to be significantly smaller than the wavelength of the radiation. To be effective, holes resulting from connections of the shield to the electronics enclosure and connectors may also need to be made smaller than the wavelength of the radiation, whether a solid or mesh conductor is utilized. The holes in the mesh may allow for the passage of wires between the power coupler and the electronics. Thus, EMI from the electronics portion of the induction lamp may be contained. EMI sourced from the power coupler may require other means as described herein.

The conductive EMI of an RF light source (also referred herein as an RF lamp or lamp) is originated by the lamp RF potential V_p on the lamp surface inducing an RF current I_g to the ac line as displacement RF current through the lamp capacitance C to free space (Earth ground) according to the expression:

I _g =V _p2πfC

where: V_p is the lamp surface RF potential, and f is the lamp driving frequency. The lamp capacitance can be evaluated in the Gaussian system as equal to the lamp effective radius R, C=R in cm or in the SI system as 1.11 R in pF. For an RF lamp size of A19 this capacitance is estimated as about 4 pF; that results in V_p=1 V corresponding to existing regulation limit at 2.65 MHz.

The value of the lamp RF potential V_p is defined by capacitive coupling between the RF carrying conductors (mainly the winding of the lamp coupler and associated wire leads) and the discharge plasma in the lamp envelope on the opposite side of re-entrant cavity from that housing the lamp coupler.

The EMI compliance is especially problematic for integrated, self-ballasted compact RF lamps. The requirements for these compact RF lamps are much stronger, since they are connected to ac line directly through a lamp socket and have no special dedicated connection to earth ground, as is the case for powerful RF lamps having remote grounded ballasts.

One effective way to reduce the RF lamp potential is to use a bifilar coupler winding consisting of two equal length wire windings wound in parallel, and having their grounded ends on the opposite sides of the coupler.

The essence of this technique is the RF balancing of the coupler with two non-grounded wires on the coupler ends having equal RF potential but opposite phase. Such balancing of the coupler provides compensation by means of opposite phase voltages induced on the re-entrant cavity surface, and thus, on the plasma and the lamp surface.

Although this technique for reduction of conductive EMI has significantly reduced the lamp RF voltage and has been implemented in many commercial RF induction lamps, it appeared that is not enough to comply with the regulation. Some additional means are needed to farther reduce the EMI level to pass the regulations.

In embodiments, a pair of closely spaced, parallel windings may be bifilarly wound on the core of the coupler. As described herein, the first winding may be an active (or driven) winding 1120, and as such, connected to the ballast 1136 with its RF end 1126 and its grounded end 1130. RF current in the first active winding creates an RF magnetic field in the core that in turn induces the time-varying electric field that maintains the discharge plasma in the lamp burner.

The second winding may be a passive winding 1122, having the function of developing the opposite (in reference to the first winding 1120) phase voltage on the coupler 110, (thereby reducing the lamp conductive EMI). The passive winding 1122 may be connected to the ballast 1136 with its grounded end wire 1132, leaving its other end free.

In embodiments, the individual turns of the bifilar winding may be positioned with space between the individual turns. In embodiments, the bifilar coupler winding may be wound such that the first and second windings are wound in close proximity to one another.

In one of the embodiments, the turns of wire on the coupler are evenly spaced. Spacing distance is chosen to achieve desired inductance and mix of combined magnetic field 4002 effect as shown in FIG. 40 relative to magnetic field effect around individual wires. In an exemplary embodiment, the even spacing of the turns of wire on the coupler core is achieved by winding three wires in parallel on the coupler core as showing FIG. 41. One wire is the electrically conductive active wire 1120 carrying the time-varying electric current, a second “wire,” or spacer tube 4102 comprises an electrically inert material such as Teflon or plastic that acts to separate the turns of the coil and a third passive electrically conductive wire 1122 acts to counter the electric field and radio interference or EMI generated by the time-varying electric field of the first wire. The outer diameter of the electrically inert “wire,” or spacer tube 4102 may be selected to achieve the desired spacing between the turns of the electrically conductive wire carrying the time-varying electric current. In one embodiment, the gauge of the electrically inert “wire,” or spacer tube 4102 is AWG28 thin wall, resulting in an outer diameter of 0.036 inches.

In another embodiment, the spacing between the turns of wire on the coupler is variable. For instance, the spacing between turns may be larger at the ends of the coupler than in the middle, such as shown in FIG. 42A. Alternately, the spacing between the turns of wire may be larger in the middle and more closely spaced at the ends of the coupler, such as shown in FIG. 42B. These figures and descriptions are meant to be illustrative and are in no way limiting. The spacing of the turns may also be random, as a method of cancelling EMI. Varying the spacing of the turns of the wire along the coupler may be a means to generate a magnetic and electrical field in the burner envelope that varies in maximum intensity along the length of the coupler. This may be used to accommodate variations in the shape of the burner envelope; increasing the maximum induced magnetic and electric fields where the bulb is widest and a larger field is needed and minimizing the maximum induced magnetic and electric fields in areas where the burner envelope is more narrow and a smaller field is needed.

In one embodiment of the invention, as shown in FIG. 12B, the end of the RF source 1136 that is not connected to circuit common is electrically connected to the turns of wire along the coupler at the end of the coupler closest to the ballast. This results in the end of the coupler with the highest voltage relative to ballast circuit common, V_max, occurring at the end of the coupler exiting the re-entrant cavity. Alternately, the high potential side of the RF source 1136 is electrically connected to the turns of wire along the coupler at the end farthest from the ballast as shown in FIG. 43. This results in V_max occurring at the inner end of the re-entrant cavity. The positioning of V_max higher in the burner cavity may facilitate startup of the lamp.

In an alternate embodiment, the individual turns of the bifilar winding may likewise be positioned as close together as possible, such as being separated primarily by the insulation of the individual windings. The wires of the individual windings may be selected such that electrical insulation is maintained while facilitating the closest possible spacing between the wires. It is important to use insulation with high-dielectric strength so that the insulation may be kept extremely thin, as close to a bare wire as practicable while maintaining adequate electrical insulation. Spacing approaching two to six thousandths of an inch between individual windings may be achieved with insulation materials such as an enamel coating, silicone, PTFE (polytetrafluoroethylene), polyimide and the like. The windings may be positioned to achieve desired spacing using a mechanical guiding device during manufacturing, grooves in a ferrite core around which the windings are being positioned, a mechanical form inserted between a ferrite core and the windings designed to hold the wires in the desired position, a mechanical form inserted over the windings designed to hold the wires in the desired position and the like.

In this way, the overall coil length may be substantially reduced, relative to a winding with more loosely spaced turns. Referring to FIGS. 33-34, both sets of windings have the same number of turns around the core. However, in the configuration illustrated in FIG. 33, there is a gap between the turns of the bifilar coupler windings, resulting in a given overall coil length 3302 along the core, while in FIG. 34, the loops of the bifilar coupler winding are closely wound, with a minimal space between the coils, resulting in a reduced overall coil length 3402. The reduced coil length 3402, as compared to coil length 3302, results from the close spacing of the loops, and as such may result in further EMI reduction.

In order to illustrate this reduced EMI, consider that conducted EMI is proportional to the capacitance of the power coupler relative to the external environment. The capacitance of the power coupler is proportional to the area subtended by the windings of the coil. Referring to FIG. 33, a coupler is shown with five windings spaced on the core. The side surface area of a cylinder is:

A=2πrh

where

r is the radius of the coil

h is the vertical coil length 33023402 encompassed by the windings.

As the space between the windings decreases, the vertical coil length, h, will decrease as well. Thus, the area encompassed by the turns of the winding along the core decreases as the space between the windings decreases.

A decrease in total coil length (e.g., from 3302 to 3402) may contribute to a decrease in radiated EMI. In general, radiated EMI is due to the electric dipole strength of the radiator, in this case the coupler coil. The coupler coil has a potential voltage difference between the upper and lower turns of the coil due to the drop in voltage along the coupler coil due to the resistivity of the coil material. The electric dipole strength is proportional to the product of the length of the coil times the potential. So by reducing the vertical length of the coil (h) from 3302 to 3402, the electric dipole strength is reduced, and thus, the radiated power at a given harmonic. For a given harmonic frequency omega (ω), the total radiated power, follows:

$P\left(\omega \right)\cong \frac{{2\left[\frac{d^2}{{\mathrm{dt}}^2}\left(h*v\left(\omega ,t\right)\right)\right]}^2}{3c^3}$

In a non-limiting example, two lamps were made each having twelve turns of a bifilar coupler winding around a ferrite core. In one lamp the turns were closely spaced, subtending a coil length 3402 of approximately nineteen mm. In the second lamp, there was a gap between the turns resulting in the coil subtending a coil length 3302 of approximately thirty-one mm. Both lamps showed similar lumen output and startup characteristics. Referring to Table 3, when both lamps were measured for radiated and conducted EMI pursuant to FCC regulations part 18 covering radio frequency consumer electronics, the lamp with the shorter coil length 3402 passed while the lamp having the longer coil length 3302 emitted higher EMI and failed.

TABLE 3
Measured Conducted EMI Relative to Coil Length
	Frequency	Limit	Peak Line 1 (dBuV)
	(MHz)	(dBuV)	19 mm coil	31 mm coil
	2.8	69.5	60.3	70.8
	5.6	48	44.8	51.5
	8.4	48	36.0	47.3
	11.2	48	35.6	37.6
	16.8	48	29.1	39.8

In embodiments, the coil may be positioned in the center of the length of the coupler. In a non-limiting example, EMI testing was conducted for a lamp having closely spaced coil windings positioned at the top, center and bottom of a ferrite core. Referring to Table 4 the coil positioned in the center of the coil exhibited the lowest conducted EMI. When the coil was further away from the ballast, toward the top of the ferrite core, the EMI was somewhat worse. When the coil was positioned near the bottom of the ferrite core, closer to the ballast, the emitted EMI was increased relative to the coil positioned at the top of the ferrite core. Thus, EMI generated when the coil is positioned on the upper two thirds of the ferrite core is reduced relative to the EMI generated when the coil is positioned on the lower third of the ferrite core. The position of the coil which minimizes EMI is approximately the center of the ferrite core.

TABLE 4
Measured EMI relative to Coil Position on Core
Frequency	Limit	Peak Line 1 (dBuV)
(MHz)	(dBuV)	Centered	Top	Bottom
2.8	69.5	65	70	72
5.6	48	44	51	57
8.4	48	39	44	47

In embodiments, a variety of EMI suppression means may be implemented, such as including a segmented electrostatic shield between the coupler and re-entrant cavity to reduce conductive EMI, a light transparent conductive coating placed between the lamp glass and phosphor, an external metal conductive coating for lamp RF screening, and the like.

An alternative (to bifilar winding) way to balance RF coupler has been proposed for RF balancing the coupler by winding on it two wires in the azimuthally opposite directions and to optionally drive such coupler with a symmetrical (push-pull) output ballast.

In examples, a combination of a bifilar symmetric winding with screening of the RF wire connecting the coupler with the ballast by a braided shield may provide an EMI reduction of inductive RF fluorescent lamps.

The exemplary embodiments that follow provide an RF induction lamp with simple and low cost means for suppressing electromagnetic interference. This goal may be achieved by a bifilar winding of the lamp coupler having unequal winding wire lengths. Further, an effective grounding of the coupler ferromagnetic core may be made with a conductive shell in conductive contact with the coupler ferromagnetic core. These relatively inexpensive solutions may reduce the conductive electromagnetic interference (EMI) level sufficiently to pass all existing regulations on such interference with significant reserve. In embodiments, the conductive shell may be a foil, a mesh, and the like. The conductive ‘shell’ may be implemented as one or of a plurality of conductive strips. The conductive shell, in contact with the coupler ferromagnetic core, may be located inside the ferromagnetic core (e.g. inserted into a cavity within the ferromagnetic core), located between the ferromagnetic core and the coupler windings, located such that a portion of the conductive shell wraps over the coupler windings on the side of the windings opposite the ferromagnetic core, and the like, or any combination thereof.

For example, the conductive shell may be a sheet of conductive foil located between the windings and the ferromagnetic core, with the conductive foil having a strip that wraps over the windings and down along the top of the windings, such as axially down the power coupler. FIG. 21 shows a front view 2100 and a cross-sectional side view 2101 of a power coupler with a representative conductive material (e.g., a conductive foil) 2110 located with an inner portion 2112 inside a hollow interior 2104 of the ferromagnetic core 2102, and wrapped over and around to the exterior of the power coupler such that an outer portion 2114 is located across at least one of the windings 2108. In this example, the outer portion 2114 is configured as a single strip of conducting foil, but one skilled in the art will appreciate that there are many different configurations that satisfy spirit of the embodiment, such as with a plurality of strips, a thin strip, a wire or plurality of wires, and the like, with the length of the outer portion being across one, more than one, or all of the windings. Further, the size and shape of the inner portion 2112 may similarly be a wire, a strip, a plurality of strips, a sheet, a slotted sheet, and the like. In embodiments, the conductive material 2110 may not need to be in direct electrical contact with the ferromagnetic core, where a relatively large overlapping surface of the conductive sheet and the ferromagnetic core may provide a sufficient interface to ground, as described herein.

In view of the limitations now present in the related art, a new and useful RF inductive lamp with simplified and effective means for conductive EMI suppression without lamp RF screening and shielded RF wiring is provided.

In accordance with exemplary and non-limiting embodiments, the lamp coupler may be wound with a bifilar winding having an unequal number of turns, in such a way that additional turns of the passive winding compensate the capacitive coupling (to the discharge plasma within the lamp envelope) of the RF connecting wire of the active winding. Due to opposite phases of RF voltages on the non-grounded ends of active and passive windings, the compensation takes place when the induced RF capacitive currents of opposite phase on the re-entrant cavity are equal or approximately equal to each other.

In accordance with exemplary and non-limiting embodiments, a grounded foil shell (tube) may be inserted into the ferromagnetic core of the coupler to reduce the coupler uncompensated common mode RF potential, where the ferromagnetic core may be a tubular ferromagnetic core. Due to the large shell surface contacting with the core and the very large dielectric constant (or large electrical conductivity) of ferromagnetic materials, the RF potential of the coupler and thus the conductive EMI created by RF lamp may be significantly reduced.

In accordance with exemplary and non-limiting embodiments, the radial position of the coupler may be fixed inside the re-entrant cavity to prevent its direct mechanical contact to the coupler, which tends to increase capacitance and, thus, tends to dramatically increase capacitive coupling and thus, conductive EMI. To provide a minimal capacitive coupling to the re-entrant cavity, the air gap between the coupler and re-entrant cavity may need to be fixed and equal over all surface of the coupler. Such fixation may be realized by means of an increased coupler diameter on its ends with an additional bonding, a ring spacer set on the coupler ends, and the like.

In accordance with exemplary and non-limiting embodiments, a spatially stable position of the connecting RF wire in the volume outside of the ballast compartment may be provided by mechanical fixing the wires on the inside of the lamp body. Such measure would keep the capacitance of the RF connecting wire to the re-entrant cavity at a fixed value during lamp assembling and reassembling.

FIG. 11 illustrates a cross-section view of an inductive RF lamp in accordance with an exemplary and non-limiting embodiment. The RF lamp 1110 comprises of a glass envelope 1112 with a glass re-entrant cavity 1114 sealed into the envelope 1112 and forming a gas discharge vessel (burner) between them. The lamp burner is filled with a working gas mixture of a noble gas such as Argon, Krypton or others and Mercury vapor. The inner surface of burner, both the envelope 1112 and the re-entrant cavity 1114, are covered with a phosphor. With plasma discharge maintained in the burner, the UV radiation from plasma excites the phosphor, which converts UV light to visible light.

The plasma within the burner is maintained by the electric field created by time-varying magnetic field created by the RF lamp coupler 110 sitting inside the re-entrant cavity 1114. The coupler 110, comprising a core 1118 and winding(s) 1120, 1122, is energized by an RF power source (RF ballast) 1136 placed in the ballast cap 1134 and electrically connected to the local ground (buss), where the ballast cap 1134 may be either non-conductive or conductive with a non-conductive coating on the outside to prevent electrical shock. In this embodiment, the coupler 110 consists of a ferromagnetic core 1118 that may be a ferrite with high magnetic relative permeability r>>1, such as where r is between 20 and 2000. For the frequency of 2.51 MHz to 3.0 MHz allocated for RF lighting, the preferred material may be Ni—Zn ferrite with relative permeability r around 100 having high Curie temperature T_c>300° C.

Two windings 1120 and 1122 may be bifilarly wound either directly on the core 1118 of the coupler 110, or with any form or spool between them. The first active winding 1120 is connected to the ballast 1136 with its RF end 1126 and its grounded end 1130. RF current in this winding creates RF magnetic induction in the core that in turn creates the time-varying electric field that maintains the discharge plasma in the lamp burner.

The second, passive, winding 1122 has the function only of inducing the opposite (reference to the first winding 1120) phase voltage on the coupler 110, (thereby reducing the lamp conductive EMI). The passive winding 1122 may be connected to the ballast 1136 only with its grounded end wire 1132, leaving its RF end free.

In embodiments, the number of turns of the passive winding 1122 may not be equal to that of the active winding 1120. Excess turns 1124 (it could be one or more turns, or a fraction of a turn) may be added to the passive winding. The purpose for addition of these excess turns 1124 is to create some additional (opposite phase) RF capacitive current to the re-entrant cavity, to compensate that induced by the RF leads 1126 of the active winding.

The general condition of such compensation (the equality of RF current induced with opposite phase) is:

∫₀^L1C₁(x)V₁(x)dx=∫₀^L2C₂(x)V₂(x)dx

Here, the integration is along the wire path x. C₁ and C₂ are the distributed capacitances correspondingly along the active winding connecting wire 1126 and the passive additional winding 1124; V₁ and V₂ are correspondingly, the distributed RF potentials along the wires, and L₁ and L₂ are correspondingly, the length of the connecting and additional winding wire.

Note that due to the three-dimensional structure of the RF lamp, with arbitrary RF wire positions, it is extremely difficult to calculate the functionalities C₁(x) and C₂(x). Therefore, the proper number of turns in the additional passive winding 1124 may have to be found empirically for a specific RF lamp embodiment.

To further reduce the common mode RF potential of the coupler 110 due to its imperfect balancing, a grounded conductive foil shell (tube) 1128 may be inserted into the tubular ferrite core 1118 of the coupler 110. Due to the shell's large surface, its close contact to the inner surface of the core 1118, and a very high ferrite core dielectric constant (or/and its high conductivity), the coupler RF potential reference to local ground is considerably reduced, and thus, conductive EMI in the RF lamp.

The shell 1128 inserted into the core 1118 may be made of a conductive foil, such as copper foil, aluminum foil, and the like. It may be made as a closed tube, have a slot along its axial direction, and the like. In the latter case, the shell may operate as a spring assuring a good mechanical contact with the inner surface of the core. The length of the shell may be equal, or somewhat longer or shorter than the length of the coupler. A larger contacting surface between the shell and the coupler will provide better grounding. On the other hand, a shell length shorter than that of coupler may be enough for adequate coupler grounding.

Grounding of the coupler with the inserted conductive shell has a certain advantage compared to grounding with an external conductive patch. Contrary to an external patch, the internal shell may not increase inter-turn capacitance and may not induce eddy current in the shell. Both these effects diminish the coupler Q-factor and consequently increase power loss in the coupler. The absence of an eddy current in the inserted shell is due to the fact that RF magnetic lines in the coupler are parallel to the shell and are diverging on the coupler ends, thus they are not crossing the foil surface.

To prevent the coupler 110 from touching the re-entrant cavity 1114, and thereby increasing conductive EMI, the coupler may need to be fixed in the approximate center and approximately equidistant of the walls of the re-entrant cavity as it is shown in FIG. 12. This may be done with a pair of spacers 1140 and 1142 placed correspondingly on the bottom open end and the upper closed ends of the coupler 110. The spacers may be made of an electrically non-conductive material, such as a fiber-reinforced polymer, fiberglass, ceramic fiber, high-temperature plastic, silicon rubber, and the like. In the case of a fiber-reinforced polymer, the fiber may be glass, carbon, basalt, aramid, asbestos, and the like, and the polymer may be epoxy, vinylester, polyester thermosetting plastic, phenol formaldehyde resins, and the like. The spacers may be rated for high-temperature, such as rated to 200° C. The top spacer 1142 may better assure axial symmetry between the coupler and reentrant cavity along with providing a cushioned secure fit of the coupler assembly against the closed end of the glass reentrant cavity. To accommodate this, the spacer 1142 may be made from a pliable material and have a shape that provides a secure mechanical interface between the coupler and the re-entrant cavity. The pliable spacer 1142 may have a shape that both provides structural support to prevent movement of the power coupler axially with respect to the re-entrant cavity and to provide axial alignment of the power coupler to the re-entrant cavity. Such a shape may include a cylinder, a cylinder with a beveled edge, a hemispherical shape, and the like. The spacer 1142 may also have a hole through the top, such as smaller than the core. In an example, as shown in FIG. 12, the spacer 1142 may be a beveled spacer 1150 with a hole through it and with a beveled edge 1154 facing into the corner of the re-entrant cavity 1114. More generally, the beveled spacer may be described as a conical frustum shape (e.g. a circular disk-like shape with a trapezoidal cross-section) where the conical frustum has two parallel surfaces of unequal surface area, and in this instance, where the smaller of the two parallel surfaces faces the closed innermost end of the re-entrant cavity. The beveled or conical frustum shaped spacer 1150 may provide a fit to the inside corner of the re-entrant cavity, thus providing greater position stability in maintaining the alignment of the coupler with respect to the re-entrant cavity. The beveled spacer 1150 may provide cushioning between the coupler and the re-entrant cavity along with an additional spacer component 1152 that aids in the alignment of the coupler and the re-entrant cavity. Alternatively, a single beveled spacer 1158 may be provided that provides both cushioning and alignment, where the single beveled spacer 1158 provides cushioning against the closed innermost end of the re-entrant cavity and position alignment from the sides of the re-entrant cavity. The bevel 1154 may provide an especially good fit to the corner of the re-entrant cavity due to the fact that the inside ‘corner’ of the re-entrant cavity may be concave in shape and where the bevel 1154 seats the spacer 1142 into this concave corner much better than would a sharp edged spacer. In embodiments, the spacer 1142 may also have a lip facing the innermost end of the coupler so as to mechanically secure the position of the power coupler with respect to the re-entrant cavity. The use of spacers 1140 and 1142 may allow for the coupler to be maintained in an axially aligned position with respect to the re-entrant cavity, thus improving EMI performance, and at the same time reducing the need for the coupler to be designed to be a stand-alone structurally rigid component, thus potentially reducing the cost of the coupler's manufacture.

It may be advantageous to have an air gap between the coupler 110 and re-entrant cavity 1114 rather than filling this space with some capsulation material having a high dielectric constant, e>>1. In the latter case, the capacitive coupling of the coupler winding to the discharge plasma on the opposite side of the re-entrant cavity from the coupler would increase by e times. Since in practice, it is impossible to reach the ideal RF balancing of the coupler, its residual common mode potential (and so EMI level) would be e times larger than that with air gap. It is found empirically that the gap between coupler windings and inner surface of re-entrant cavity of approximately 0.5-1.5 mm is enough for embodiments of the RF lamp to pass EMI regulations. Although, increasing of the air gap reduces conductive EMI, the inductive coupling efficiency and lamp starting would be deteriorated.

It was found in many experiments with non-shielded RF wire 1126 connecting the coupler 110 to ballast 1136, the conductive EMI level is extremely sensitive to the spatial position of this wire within the lamp body. An arbitrary position of this wire after the lamp assembling may diminish the effect of the measures described above towards EMI reduction in the RF lamp. Therefore, fixing the position of the wire to some lamp inner elements may be necessary. Note that wire may be needed to be fixed in position only in the space between the coupler 110 and the grounded ballast case 1134. The position of the wires inside the ballast case may not be important for conductive EMI.

As it seen in FIGS. 11 and 12, four wires 1126, 1130, 1132 and 1138 may be connected between the coupler and the ballast. Indeed, in this embodiment, three of them, 1130, 1132 and 1138 are grounded within the ballast case, and the forth is connected to the output of the RF ballast 1136. Practically, only the positioning of the RF wire 1126 is important for the EMI issue, but the grounded wires 1130 and 1132 being positioned on both side of the RF wire 1126 (as it shown in FIGS. E1 and E2) partially perform a shielding function reducing the sensitivity of the conductive EMI level to the position of the RF wire. For this purpose, the wires 1130, 1132 and between them wire 1126 may be fixed together (touching each other with minimal distance between them) on the inner lamp body, such as with some painting, a sticky tape, and the like.

Numerous experiments conducted in the laboratory showed that the exemplary embodiments considered herein are effective and inexpensive ways to address conductive EMI in an RF lamp.

Evaluation of conductive EMI levels of the exemplary embodiments described herein has been done by measurement of the lamp surface voltage Vp, which is proportional to EMI level. For instance, the maximum value of Vp corresponding to the regulation threshold for RF lamp of size A19 at 2.65 MHz, is 2.8 Volt peak-to-peak.

To measure the Vp values, the lamp glass envelope was entirely covered with thin copper foil as it shown in FIG. 13 The foil jacket had eight meridian slots to prevent its interaction with the lamp RF magnetic field. The capacitance between the foil and the plasma inside the lamp burner was estimated as a few hundred pF, which was much larger than the input capacitance (8 pF) of the RF probe connected between the foil and a scope.

Concurrently, a similar measurement has been done with a commercial lamp having the same size of A19 (6 cm diameter), where the intent was to compare the EMI performance of the commercial lamp to a lamp constructed consistent with exemplary embodiments described above. Since the results of the measurements were dependent on lamp run-up time, the measurements for both lamps were performed at the same time with a two-channel oscilloscope. The experimental set-up for measurement of the lamp surface voltage Vp is shown in FIG. 14. The 22 kQ resistor is used to prevent line frequency interference with the measurement of small RF voltages. The overall test set up was provided by the international standard on EMI test equipment, CISPR 16. Power was provided to the test lamp through a Line Impedance Stabilization Network (LISN). This network collected the EMI noise on each power line (120V and Neutral) and routed the collected EMI to a measurement analyzer. In this case, a spectrum analyzer that was specifically designed for EMI measurements was used.

In the U.S., the Federal Communications Commission (FCC) writes the rules for EMI compliance. These lamps are required to comply with FCC Part 18. There are several compliance requirements including technical and non-technical requirements, but only the FCC-specified residential market limits for EMI were used in this coupler comparison. Testing of the noise on the power line was done over the range of frequencies from 450 kHz to 30 MHz in accordance with FCC Part 18 requirements. The lamps were mounted in an open-air fixture with their bases oriented downward. The warm up times from a cold turn-on were kept the same at one hour. A peak detector (PK) was used to speed up the testing. The plots of measured data show limit lines that apply when a quasi-peak detector (QP) is used. For this lamp, QP data is typically 3 dB lower than the PK data. So if the PK data is below the limit line, the QP data will be even lower and doesn't need to be measured. Typically, in EMI testing, PK data is recorded initially, and QP data is measured if the PK data is near or over the limit line. For this comparison task, measuring PK data allows the two couplers to be compared.

FIGS. 15 and 16 show the FCC Part 18 limit line on plots of measured data for the two lamps. The horizontal axes are frequency in MHz and the vertical axes are the amplitudes of the measured EMI on a log scale in units of dBuV, or dB above 1 uV. The construction of couplers impacts the response vs. frequency, and the two different couplers were not expected to have identical EMI patterns vs. frequency. What is important is that both couplers have relatively low EMI that is capable of complying with the FCC's technical limits for Part 18 EMI. Although not shown, couplers without EMI reducing features will exceed the FCC's limits considerably. The main operating frequency of the electronic circuit powering the coupler is near a frequency of 2.75 MHz. As shown there is a “chimney” on the limit line between 2.51 and 3.0 MHz. where increased EMI is allowed. It should be noted that in this chimney, the generated EMI could be quite large. Exemplary embodiments lower the EMI in this chimney, as shown in FIG. 16 relative to that shown in FIG. 15.

The results of different steps discussed above were separately tested on this set-up, and confirmed for their effectiveness. When these steps were incorporated together in the final RF lamp embodiment, its EMI level was similar to that of the commercial lamp, and both were considerably lower than the regulation threshold. Thus, the measured values of the lamp surface voltage, for the newly invented lamp and commercial one were 0.58 V and 0.48 V peak-to-peak respectively, values well under the required limitations from the FCC for conductive EMI.

Referring to FIGS. 12A and 12B, in certain situations it may be desirable to connect the coupler 110 to RF ground through a capacitor 1144 that has a low impedance at the operating frequency of the lamp, but a high impedance at the frequency of the AC power line. This would prevent electrical shock if a human came in contact with an exposed coupler 110 while the lamp was connected to an AC power line, even if the high frequency converter in the ballast was not operating. The term “RF ground” is understood to mean any node of the ballast that has a low RF potential with respect to the circuit common node. In a typical ballast, both the circuit common, which is typically the negative DC bus, and the positive DC bus, are RF ground nodes. Referring to FIG. 12A, in embodiments, the coupler 110 may include a ferromagnetic core 18, and the connection of the capacitor 1144 may be made to the coupler 110 or to any component associated with the coupler 110, such as a ferromagnetic core, a conductive foil or shell inserted within or around the core, and the like. Referring to FIG. 12B, in embodiments, the coupler 110 may include an air-core, and the connection of the capacitor 1144 may be made to the coupler 110, such as directly to the winding return 1130, and the like. In embodiments, there may be two capacitors connected to the winding, such as one capacitor connected at one location (e.g. at a first end of the winding) and a second capacitor connected at a second location (e.g. at the second end of the winding). The coupler 110 of FIG. 12B is shown with a dotted line to indicate, as described herein, that an air-core coupler may optionally include a non-magnetic and non-conductive supporting material, such as a plastic form, to support the conductor coil, or, if the coil is self-supporting, with no additional support at all.

The potential for electrical shock may arise when an electronic circuit is powered from an AC power line by means of a full wave bridge rectifier because the magnitude of the voltage difference between the positive output terminal of the full wave bridge rectifier, which is normally connected to the positive DC bus of the high frequency converter, and each of the two AC power lines will periodically be equal to the peak of the AC input voltage between those two power lines. In like manner, the magnitude of the voltage difference between the negative output terminal of the full wave bridge rectifier, which is normally connected to the negative DC bus of the converter, often labeled circuit common, and each of the two AC power lines will also periodically be equal to the peak of the AC input voltage between those two power lines. Due to this characteristic of circuits powered from AC power lines through full wave bridge rectifiers, the potential for electric shock exists if users are allowed to come in contact with circuit common or other node of the circuit that does not have a high impedance to circuit common at a frequency of 60 Hz. For instance, and without limitation, if the conductive foil shell 1128 shown in FIG. 11 is connected directly to any point in the ballast circuit, a potential for electrical shock is created if users come in contact with the ferrite core 1118 of coupler 110.

In order to remove such a shock hazard, the low resistance connection between the coupler 110 and ballast circuitry should be removed and replaced with a capacitor 1144 that has a low impedance at the operating frequency of the lamp and a high impedance at the power line frequency.

In a non-limiting example, and referring to FIG. 12A, for a lamp operating frequency of 2.65 MHz with a ferromagnetic core with conductive foil shell inserted, and operated from a 60 Hz power line, the isolation capacitor should have a value between 0.6 nF and 13 nF, where we want the 60 Hz leakage current from the ferrite core 1118 to earth ground be no greater than 1 mA, and the magnitude of the impedance from the conductive foil shell to circuit common, or to the positive DC bus, at the lamp operating frequency of 2.65 MHz to be no higher than 100 Ohms. The magnitude of the impedance of a 0.6 nF capacitor is 100 Ohms at 2.65 MHz and 4.4 Meg Ohms at 60 Hz. The magnitude of the impedance of an 11 nF capacitor is 4.62 Ohms at 2.65 MHz and 200 K Ohms at 60 Hz. Different capacitor values can be used if these boundary conditions are relaxed.

In a different non-limiting example, and referring to FIG. 12B, for a lamp operating frequency of about 27 MHz with an air-core coupler, and operated from a 60 Hz power line, the isolation capacitor should have a value between 60 pF and 13 nF, where we want the 60 Hz leakage current from the coupler 110 to earth ground be no greater than 1 mA, and the magnitude of the impedance from the coupler to circuit common, or to the positive DC bus, at the lamp operating frequency of about 27 MHz to be no higher than 100 Ohms. The magnitude of the impedance of a 60 pF capacitor is 98 Ohms at 27 MHz and 44 Meg Ohms at 60 Hz. The magnitude of the impedance of an 11 nF capacitor is 0.453 Ohms at 27 MHz and 200 K Ohms at 60 Hz. Different capacitor values can be used if these boundary conditions are relaxed.

Optics

In embodiments, optical coatings may be used to optimize the performance of the induction lamp, such as to maximize visible light emitted, minimize light absorbed by the power coupler, and the like. Optical coatings may at least partially reflect, refract, and diffuse light. For instance, a reflection coating may be used to reflect light impinging on the re-entrant cavity back into the burner, as otherwise that light may be absorbed by the coupler and thus not converted to visible light emitted to the external environment. Further, light absorbed by the coupler may contribute unwanted heat to the coupler, thus affecting its performance, life, and the like. In another instance, optical coatings may be used on the outside envelope of the burner, such as between the phosphor coating and the glass, where this optical coating may enhance the transfer of light through the glass, such as though index matching. Further, the coating may be used to help decrease absorption of the mercury into or onto the glass envelope. Optical coatings may also be used to create or enhance aesthetic aspects of the induction lamp, such as to create an appearance for the lower portion of the induction lamp to substantially look like the glass upper portion of the induction lamp. In embodiments, coatings on the upper and lower portions of the induction lamp may be applied so as to minimize the difference in the outward appearance of the upper and lower portions of the induction lamp, such as to minimize the differences in the outward appearance of the induction lamp to that of a traditional incandescent lamp, thus creating a more familiar device to the consumer along with a resulting increase in usage acceptance with respect to being used for replacement of incandescent lamps.

In embodiments, optical components may be provided to enhance a lighting property of the induction lamp. Optical components may include reflectors, lenses, diffusers, and the like. Lighting properties affected by optical components may include directionality, intensity, quality (e.g. as perceived as ‘hard’ or ‘soft’), spectral profile, and the like. Optical components may be integrated with the induction lamp, included in a lighting fixture that houses the induction lamp, and the like. For instance, reflectors and lenses may be used in a lighting fixture in conjunction with the induction lamp to accommodate a lighting application, such as directional down lighting, omnidirectional lighting, pathway lighting, and the like. In an example, a lighting fixture may be created for a directional down light application, where reflectors proximate to the sides of the induction light direct side light from the induction lamp to a downward direction, where a lens may further direct the light reflected from the reflected side light and directly from the induction lamp within a desired downward solid angle.

Electronic Ballast Having Improved Power Factor and Total Harmonic Distortion

In embodiments, as shown in FIG. 17, a source of AC voltage 120V, 60 Hz is applied to the full wave bridge rectifier BR 1702 via EMI filter F 1704, the DC output voltage of BR is applied directly between the positive rail +B 1708 and negative rail −B 1710 of the DC bus which is coupled to the output of BR. There is no traditional energy-storage electrolytic capacitor across DC bus. A DC backup voltage generated by the Passive Valley Fill Circuit (PVFC) 1722 is superposed on the rectified voltage and results in Vbus voltage for powering a high frequency resonant inverter INV 1712. A small bypass capacitor Cbp 1714 is connected to the input of the DC inverter to smooth out high frequency voltage ripple generated by the resonant inverter INV. The resonant inverter INV powers a fluorescent lamp 1718. Multiple lamps may be powered from a single inverter INV (not shown in FIG. 17). The inverter INV may have a control circuitry C 1720 for driving power stages and other needs. This circuitry needs an auxiliary power supply. In FIG. 17 the auxiliary power is obtained from the 4-capacitor 9-diode (4C9D) PVFC via a resistor R11724. The PVFC is a network built with four small capacitors, each having a voltage rating substantially below the voltage of the DC bus, and 9 diodes for generating a backup DC voltage that is about ¼^th of the peak rectified voltage. For a 120V AC line this DC voltage will be about 40V. This voltage is sufficient to support continuous lamp operation. The PVFC comprises first, second, third, and fourth capacitors, designated C11741, C21742, C31743, and C41744, each having a positive terminal designated as “+” and also having a negative terminal. These capacitors are connected in series via first, second and third charge diodes designated as D11731, D21732, and D31733, each having an anode and a cathode. The diodes D1, D2, and D3 allow capacitors C1, C2, C3 and C4 to charge in series, but prevent those same capacitors C1, C2, C3, and C4 from discharging in series. Passive Valley Fill Circuit PVFC also comprises fourth, fifth, sixth, seventh, eighth and ninth discharge diodes designated in FIG. 17 as D41734, D51735, D61736, D71737, D81738, and D91739, each having an anode and a cathode. These discharge diodes provide parallel discharge paths to the DC bus for capacitor C1, C2, C3, and C4. The first charge capacitor C1 has its positive terminal connected to DC bus positive rail +B and has its negative terminal connected to the anode of the first diode D1. The second capacitor C2 has its positive terminal connected to the cathode of the first diode D1 and its negative terminal connected to the anode of the second diode D2. The third capacitor C3 has its positive terminal connected to the cathode of the second diode D2 and its negative terminal connected to the anode of the third diode D3. The fourth capacitor C4 has its positive terminal connected to the cathode of the third diode D3 and its negative terminal connected to the DC bus negative rail, −B. The cathode of the forth diode D4 is connected to the negative terminal of the first capacitor, C1, and its anode is connected to DC bus negative rail −B. The cathode of the fifth diode D5 is connected to the DC bus positive rail, +B, and its anode is connected to the positive terminal of the second capacitor C2. The cathode of the sixth diode D6 is connected to the negative terminal of the second capacitor C2 and its anode is connected to the DC bus negative rail −B.

The anode of the seventh diode D7 is connected to the positive terminal of the third capacitor C3 and its cathode connected to the DC bus positive rail, +B. The anode of the eighth diode D8 is connected to the positive terminal of the fourth capacitor C4 and its cathode is connected to the DC bus positive rail, +B. The anode of the ninth diode D9 is connected to the DC bus negative rail −B and its cathode is connected to the negative terminal of the third capacitor C3.

In embodiments, as illustrated in FIG. 19, the 4C9D PVFC 1722 (comprising C11741, C21742, C31743, C41744, D11731, D21732, D31733, D41734, D51735, D61736, D71737, D81738, and D91739) is utilized in combination with a TRIAC dimmer DM 1902, which is connected between the AC line 1904 and the input of the ballast 1908. The special features of the 4C9D PVFC is that this circuit eliminates interruptions of current flow from the AC line that cause flicker in the lamp.

With reference to FIG. 17, the operation of the ballast 1908 may be explained as follows. When the AC switch (not shown) is turned “on”, AC power is applied directly to the bridge rectifier BR 1702. There is no traditional electrolytic capacitor at the output of the rectifier, so that the inverter INV 1712 is powered from unsmoothed rectified voltage. However, the inverter INV may provide a significant lamp starting voltage when the DC bus voltage is near the peak of the AC line voltage and thereby start the lamp 1718 for at least 1-2 msec. Series capacitors C1-C4 are charged from the DC bus directly through diodes D1 to D3. Inrush current is limited by the impedance of EMI filter F 1704 and series resistance of the series capacitors C1-C4. In a quarter of the power line voltage cycle, each of capacitors C1 to C4 is charged to a DC voltage that is about of ¼th of AC peak voltage (40V DC at 120V AC power line). Current to the inverter INV will be provided either from the AC line or from capacitors C1-C4 when they discharge in parallel, depending on which of the instantaneous voltages is higher. When the instantaneous AC line voltage is above 40-45V, current will be drawn from the AC line. The current conduction angle in the bridge rectifier BR of the ballast is higher than in prior art Passive Valley Fill circuits.

FIG. 18 demonstrates actual oscillograms of the input AC line current and DC bus voltage in the ballast circuit of FIG. 17 after starting in steady-state mode. A power factor PF=0.96-097 can be achieved for ballasts driving gas discharge lamps.

Referring to FIG. 19, a system is provided that includes an electronic ballast with the 4C9D PVFC and TRIAC dimmer (such as a wall dimmer) placed in between the power line and the input terminal of the ballast. When the dimmer TRIAC turns on, all four capacitors C1-C4 are charged in series. Therefore, in the absence of an electrolytic capacitor directly connected to the DC bus, the inverter INV consumption current provides for the TRIAC holding current. This current can satisfy a commercial dimmer to keep it in the “on” position. Thus, light flickering caused by turning on and off the dimmer TRIAC is avoided. When the instant AC voltage becomes lower than the capacitor voltage, the Bridge Rectifier BR is backed up and the inverter INV is supplied by discharge current of capacitors C1-C4. The TRIAC loses its holding current and automatically turns off until the next half period. But the gas discharge in the lamp continues at a reduced power, so that with new pulses coming from the dimmer, the lamp does not need to restart. FIG. 20 demonstrates input AC current and DC bus voltage waveforms with the TRIAC dimmer at 50% “on”. The system in FIG. 19 features a wider dimming range than prior art ballasts. For 16-20 W gas discharge lamps, 22 uV, 63V capacitors values for C1-C4 may provide a dimming range down to approximately 10%. Diodes D1-D9 may be selected to be the same type. Small signal diodes and diode arrays may be used for cost and space saving.

Embodiment G25-Like Induction Bulb

Referring to FIG. 48, the induction lamp may have the approximate shape and dimensions of an ordinary G25 shaped incandescent bulb, with a dimension D_B-G25 at the widest point of the bulbous portion 4802 being within the NEMA ANSI standards for electric lamps, which sets forth the physical and electrical characteristics of the group of incandescent lamps that have G and similar bulb shapes with E26 medium screw bases. The NEMA ANSI C78.20-2003 standard for electric lamps is incorporated herein in its entirety. Although the standard provides the outer most bounds for the specified lamps, the common dimensions for said specified bulbs may be substantially within these ranges. Thus, the dimensionality of the induction lamp may be approximately equivalent to those of the ordinary incandescent bulb as manufactured as opposed to the maximum dimensions as specified in the standard, thereby effectively providing a replacement for an ordinary incandescent bulb that matches the user's expectation of the profile and size of an ordinary incandescent bulb. For example, the induction lamp may have dimensions of a typical incandescent G25 bulb, where a typical incandescent lamp has a width D_B-G25 of approximately 79.4 mm (or approximately 3.1 inches, where ‘G25’ refers to a ‘G’ profile width D_B-G25 of 25 times ⅛ inch) and height D_H-G25 of approximately 106.7 mm (or approximately 4.2 inches).

In embodiments, the lower portion 4806 may take the form of a tapered neck that has a maximum diameter substantially less than D_B-G25 into which the upper portion 4802 may be seated, such as at an upper-lower interface point 4804. In embodiments, the lower portion 4806 may be angled down to meet the electrical socket 138, such as illustrated in FIG. 48. In embodiments, the upper portion 4802 and lower portion 4806 may be connected in a manner that makes their separation less noticeable or indistinguishable to the viewer, such as by using appropriate overlay or coating materials, or by fashioning a seamless connection between the two portions. For instance, the reflective properties of the material and/or coating selected for the lower portion 4806 may match the reflective properties of the upper portion when the lamp is not powered such that the upper and lower portions appear to be materially the same. In another embodiment, the upper portion 4802 may transition completely down to the electrical socket 138, where there is no lower portion 4806.

FIG. 49A depicts an embodiment layout of the components of the RF induction within a G25 profile. In this example embodiment, the power coupler 4902A is shown approximately centered within the upper portion 4802, with the ballast electronics located below, including where the ballast electronics extend upward into the volume of the upper portion 4802. The location of the ballast electronics at least in part within the upper portion 4802 contribute to the reduction in size of the lower portion dimensions, which permit a smaller, less noticeable, lower portion 4806. In this embodiment, the induction lamp electronics are divided into an inverter electronics board 4910 and a rectifier electronics board 4914, with thermal management in part enabled with a lateral heat spreader 4906 in contact with the inverter electronics board 4910. This two-board configuration permits a layered EMI shielding configuration, with an upper EMC shield 4904 mounted between the power coupler and the electronics (completely covering all of the electronics, as illustrated), and a lower EMI shield 4908 located between the inverter electronics board 4910 and the rectifier electronics board 4914 (completely covering the rectifier electronics, and utilizing the metallic electrical socket 138 as a lower portion of the lower shielding configuration). This EMI shell 4908 within a second lower EMI shell 4908 may greatly reduce EMI for the induction lamp. FIG. 49B shows an alternate embodiment configuration, with a smaller diameter power coupler 4902B.

In embodiments, the electromagnetic shields 4904 and 4908 may be formed by using a metal core printed circuit board (MCPCB), which is press-fit into a lateral heat spreader 4906, and capped from above by another conductive disk (top cap). The MCPCB facilitates heat (electronic power losses) transfer from the components of the inverter electronics board 4910 to the lateral heat spreader 4906. The effectiveness of the electromagnetic shield is due at least in part to the continuity of the conductive assembly from below (metal core of the inverter PCB), laterally (heat spread), and from above (EMC metal top cap), which are all connected to either VC− or VC+ of the inverter electronics board 4910. The latter also provides electromagnetic shielding between the power coupler and the rectifier electronics board 4914. The inverter circuit board layout may prioritize lowest impedance paths for RF commutation currents, which maximizes the effectiveness of dc-bus bypass capacitors.

Improvements to Luminous Output

As described further herein, the upper portion 4802 is the light providing portion of the induction lamp, including a burner envelope with the power coupler 4902A-B inserted up into a re-entrant cavity, where the induction power coupler, powered by the ballast electronics, creates the time-varying magnetic field that, in turn, creates the time-varying electric field within the burner envelop. The burner envelope contains a working gas mixture. The atoms in the working gas mixture are then both ionized and excited by the time-varying electric field. The excited working gas atoms emit small amounts of visible light plus much larger amounts of ultraviolet energy that is then converted into visible light by a phosphor coating on the inside of the burner envelope, thus the induction lamp provides light to the outside environment.

The burner envelope of fluorescent and electrodeless fluorescent lamps is generally comprised of two pieces of glass, which are sealed together and filled with the appropriate gases and pressures. Generally, the sealing process involves high temperature flames, but may also be conducted using laser welding techniques. Whether the glass sealing process is performed by a flame or by a laser, care must be taken to remove the coatings from the edge of the seal. Failure to have a clean glass surface for sealing results in a poor seal or eventual lamp failure. Because a laser can control the glass temperature more accurately (using both spatial and temporal controls), a narrower welded glass seal can be produced. The result of the narrower seal is to prevent light from escaping through uncoated portions of the glass shell, which results in a loss in lumens and lumen efficiency. However, because the cost of controlling a laser for high-volume production glass welding can be high, an alternative approach for improving lumen output and lumen efficiency was also considered.

In order to create a good glass seal, the coatings are typically removed from the glass surfaces in the area where the seal will be made. While removing the coatings from the glass surface helps in producing an air-tight vacuum seal, a considerable portion of the bulb's surface area is left without phosphor coatings. This results in a loss of lamp surface area for converting UV radiation to visible light and a further loss of visible light absorbed in the lamp's base. For example, the burner configuration illustrated in FIGS. 49A-B shows the upper portion 4802 partially covered by an over-molded plastic housing of the lower portion 4806, which is where the seal would be located for cosmetic reasons. Significant light can escape from the seal region to be wasted in the lower portion 4806. However, if the location of the seal is moved away from the phosphor coating, so that the phosphor coated surfaces come together in close proximity inside the burner and the phosphor-free sealing surfaces are thereby outside of the area of UV light exposure, an air-tight vacuum seal can be made while preventing light loss through the seal region. This has been shown to increase lumen efficiency by 5-10%. FIG. 50 depicts an embodiment burner envelop with a remote glass sealing configuration 5002. In this remote glass sealing method, almost all of the burner envelope inner surface is coated with phosphor, hence the entire surface area of the lamp is capable of down-converting UV radiation to visible light. Thus, an increase in lumens and lumen efficiency equal to the percent uncoated surface area is gained in lumen efficiency.

Lumen maintenance is the measure of lumen performance over time, and is an important aspect of lamp design for providing long working life and meeting regulatory requirements. Fluorescent lamps are prone to losses in luminosity over time due to various degradation mechanisms. These degradation mechanisms may include: darkening of the phosphor coating by the deposition of elemental mercury or the formation of mercury oxide(s); damage to the phosphor by chemical reaction or ion migration from the vitreous material of the burner envelope; damage to the phosphor from chemical reaction with the working gas mixture; damage to the phosphor by ion bombardment from the plasma discharge of the working gas mixture; and damage to the phosphor by ultraviolet radiation. These lumen losses may be reduced significantly by coating the internal lamp vessel surface with metal oxide(s) such as aluminum oxide or silicon dioxide, before and/or after application of the phosphor coating. The purpose of these oxide powder coatings is to prevent reactions between the interior wall of the burner envelope, the phosphor coating, and/or the vaporized mercury or other working gas mixtures. The oxide powder coatings can reduce the detrimental deposition of compounds such as elemental mercury from the working gas mixture onto the phosphor coating layer. The oxide powder coatings can reduce or eliminate damage to the phosphor from ion bombardment or short-wavelength UV radiation from the plasma discharge of the working gas mixture.

The effectiveness of the glass coating of the metal oxide(s) can be significantly increased by depositing a nanometer-sized particle coating. For best performance, the coating should be uniform, continuous, and free of defects or pinholes. Since nanoparticles have a tendency to agglomerate during dispersion and coating, it can be difficult to produce a bonafide nano-particulate powder coating. Aqueous pre-dispersed nano-particulate alumina dispersions are capable of producing uniform coatings without agglomeration, and can be effective in protecting lamps from lumen degradation.

With reference to FIG. 51, although a first coating of metal oxide 5104 between the inner surface 5102 of the burner envelope and the phosphor coating 5106 may protect the phosphor from reaction with the material of the vitreous enclosure, it will not protect the phosphor coating 5106 from reaction with the working gas mixture or from the deposition of mercury or other compounds. Therefore, an additional protective nano-particulate metal-oxide coating 5108 is applied after the phosphor coating 5106. This guarantees that both the glass and the phosphor will have the same protection against reactions with the working gas mixture and mercury depositions.

An example system includes a vitreous portion of the fluorescent lamp comprising a vitreous envelope filled with a working gas mixture, the vitreous envelope having an inner surface facing the working gas mixture side of the vitreous portion; a first coating deposited on the inner surface, the first coating comprising a first metal oxide; a second coating deposited on top of the first coating, the second coating comprising a phosphor; and a third coating deposited on top of the second coating, the third coating comprising a second metal oxide.

One or more certain further aspects of the example system may be incorporated in certain embodiments. The first and third coatings of metal oxide may envelop the second coating of phosphor and decrease the reaction of the working gas mixture with the phosphor and the inner surface of the vitreous envelope. At least one of the first coating and second coating may be aluminum oxide, silicon dioxide, and the like. The first coating may protect the inner surface from reaction with chemicals from the working gas mixture and protect the second coating of phosphor from reaction with chemicals from the vitreous material of the inner surface. The first coating may protect the inner surface from deposition of chemicals from the working gas mixture onto the inner surface. The third coating may protect the phosphor from chemical reaction of the working gas mixture or plasma discharge with the phosphor. The coatings may be baked or fired at elevated temperature to improve adhesion of the coatings and prevent them from being removed during subsequent coating steps. At least one of the coatings of metal oxide and phosphor may be applied with a binder material to achieve more uniform coatings. The binder material may be cross-linked to facilitate the application of multiple layers without damaging or degrading previously applied layers. The binder material may be cross-linked by chemical treatment, heat treatment, or exposure to light (including ultraviolet light). One or both metal oxide coatings may be comprised of nanoparticles (e.g., as nanoparticles that are less than 1 micrometer in size), applied in the form of pre-dispersed solutions in order to achieve more complete and uniform coatings, eliminated by combining the metal oxide and phosphor particles into one coating, and the like. The third coating may protect the second coating of phosphor from being damaged by ion bombardment from the plasma discharge of the working gas mixture, from ultraviolet radiation from the plasma discharge of the working gas mixture, and the like

A further aspect of luminance output is the use of UV sources to excite ‘remote phosphors’, such as the phosphors applied to the burner envelope. Any ultraviolet light source inside the bulb can be used to illuminate a phosphor coating on the burner surface or other place where visible light production is desired. This phosphor coating converts the UV light/radiation into visible light. Many phosphors are available to convert the high energy UV photons to wavelengths across the visible (and invisible) light spectrum. This lamp construction is called “remote phosphor” because the phosphor coating is separated from the excitation light source. The benefits of remote phosphor operation are more uniformly distributed light without the use of diffusers or lenses, and lower light energy conversion per unit area. Lower light energy conversion per unit area equates to lower heat generation per unit area, which yields lower phosphor temperature, resulting in better phosphor performance and longevity. Solid-state lamps, also known as LED lamps, typically use a light emitting diode (LED) that emits visible blue photons as the starting point rather than ultraviolet light. The lower-energy blue light produced by the LED source limits the colors/wavelengths of light that these lamps can produce, since they cannot produce higher-energy purple, violet, or UV light. Also, phosphors that can convert the blue light to other colors are limited in variety and more expensive than typical UV-pumped phosphors. Therefore, the phosphors are typically coated onto the surface of the LED chips themselves rather than used in remote phosphor configurations. In addition, the blue-pumped phosphors are not white in color because they absorb visible blue light, rendering them yellowish in appearance. In embodiments, the disclosed induction lamp may utilize UV light sources (alone or in combination with visible light sources) to excite phosphor coatings, such as in the A-type, G-type, and BR-type bulb shapes as disclosed herein, such as other than through mercury plasma discharge. Such sources may include other chemistry plasma discharges, UV light emitting diodes (LEDs), cathode ray tube, field-emission cathodoluminescence UV, visible light generators, and the like.

In a further aspect of luminance output is incorporation of multiple burners into the induction lamp, such as to provide cool temperature selection. For example, one burner could run at 2700K (or lower) and one burner could run at 6000K (or higher). By dimming the two burners at different levels, the combined light could achieve any color temperature in between these extremes. A lamp fixture with a good shade or diffuser could prevent the user from seeing the two different light sources and provide uniform illumination. To make a single lamp that shifted color temperature, the induction lamp could utilize two power couplers (or two windings on one power coupler) to enable positioning the plasma discharge region within the burner. Further, by coating the finger and/or shell of the virtuous envelope with different phosphors near to the two windings, a shift in the color temperature may be achieved.

Burst-Mode Operation of RF Fluorescent Lamps

Referring to FIG. 52, an induction lamp may be pulsed in a burst operational mode to maintain stability, such as at lower power, where a timing circuit 5204 (e.g., a floating oscillator circuit), synchronously enables-disables the higher-frequency inverter circuit 5208 through an enable circuit 5206, rapidly turning the lamp on and off with off-times that are short enough that the plasma doesn't have enough time to dissipate completely while the inverter is disabled. The inverter circuit 5208, operating at a high frequency, provides voltage and current to the power coupler with reference to local ground. That is, a switching node of the inverter is connected to a first end of the winding of the power coupler, and the second end of the winding is connected to local ground. In embodiments, the timing circuit 5204, operating at a lower frequency, may be considered ‘floating’ because it operates with reference to the switching node, and the enable circuit 5206 is activated (enabled) by the timing circuit oscillation that synchronously enables and disables the inverter circuit. Thus, luminance of the lamp is driven by the high-frequency power being delivered by the inverter 5208, and the timing circuit then modulates the operation of the inverter 5208 at the frequency of the timing circuit. The ‘disabled’ period (when the self-oscillating inverter is disabled, and not providing power to the lamp) is short enough that the working gas mixture does not have enough time to dissipate completely after having been previously energized. Pulsed operation may be further improved through the use of a fast turn-on circuit and a high-Q coupler core for improved efficiency through fast re-strike at elevated coupler voltage amplitude.

FIG. 53 provides an example embodiment schematic representation for the ballast electronics of the induction lamp in an implementation of the burst operational mode, including ballast functions for an EMI filter/bridge rectifier circuit 5202, timing circuit 5204, enable circuit 5206, and inverter circuit 5208. In this example circuit representation, the timing circuit enables and disables the inverter at a much lower frequency (e.g., burst-mode operation at 1 to 2 kHz and the like), with a fixed duty cycle to produce a fixed light level. In embodiments, the circuit consists of an oscillator circuit, which is referenced to the “switch node” (as shown in FIG. 53) of the self-oscillating inverter. When the inverter is switching, the timing circuit follows the switch node voltage as it moves from VC+ to VC− in, for example, 2.5-3 MHz cycles, such as illustrated in FIG. 54. Having the entire timing circuit referenced to the switch node makes it easier to enable and disable the inverter on command, because the inverter's MOSFET gates (“gate node” as indicated in FIG. 53) are also referenced to the switch node. Other solutions which use enable/disable circuits referenced to VC− are very difficult to implement effectively, due to the gate node being very sensitive to parasitic capacitances, due to the fast rates of voltage change on the switch node and gate node while the self-oscillating inverter is running.

The timing circuit 5204 uses the output of the oscillator to alternately activate and de-activate Q5: when activated, Q5 prevents the gate node voltage from rising above the switch node voltage, and therefore prevents Q1 from turning on and disables the inverter. When Q5 is de-activated, the timing circuit no longer affects the inverter, which runs and generates light. D2 prevents the body diode of Q5 from taking effect while Q5 is off; this would prevent the gate node voltage from going below the switch node voltage, and therefore prevent Q2 from ever turning on and prevent the inverter from running. The oscillator circuit requires a low supply voltage to operate (labeled as “Vosc”). This is provided by the combination of R1 and the two components labeled “supply section”. Zener diode D1 regulates Vosc, while the capacitor keeps Vosc stable during switching. R1, a large-value resistor, allows a small amount of current to flow from VC+ to the timing circuit to supply Vosc. When the inverter is enabled (Q5 off), the switch node voltage is near VC+ approximately 50% of the time, and near VC− approximately 50% of the time. While the switch node is near VC+, the voltage across R1 is almost zero and it supplies no current to the floating oscillator. While the switch node is near VC−, however, the voltage across R1 is almost equal to the DC link voltage, and a small amount of current flows through it to supply Vosc. When the inverter is disabled (Q5 on), a voltage divider is formed by R1, R2, and R3 which holds the switch node voltage at some point between VC− and VC+. During this time, the voltage across R1 is almost equal to the difference between VC+ and the switch node voltage, and some current flows through R1 and supplies Vosc. A smaller value of R1 allows more current to flow to the floating oscillator circuit, and is required if the current draw of Vosc increases. More power is dissipated in R1 as its value is decreased, however.

Additionally, Zener diodes may be applied as clamping devices across capacitive and inductive elements in order to limit transient effects of inverter repetitive restarting. The inverter circuit 5208 operates based on a positive feedback process, where a signal from part of the inverter output network provides the control signal for Q1 and Q2. The amplitude and phase of the feedback signal are critical requirements needed to ensure that the feedback signal propagates through the inverter, in order to sustain operation. Specifically, the loopgain frequency response of the inverter must have magnitude greater than one, and 360 degrees delay. The output voltage of the rectifier is a multiplicative factor in the loopgain. If the rectifier output voltage falls too low, the loopgain loses gain margin, and risks failure to oscillate. This is prevented by the Zener diode clamp, so that output inductor is prevented from resonating, which furthermore mitigates sags in the output voltage of the rectifier. Mitigating unwanted transistor oscillations associated with Q₁ and Q2 helps to also eliminate electromagnetic interference emissions. This is achieved by introducing an inductor or resistor in series with the gate of these transistors. The inductor characteristics must increase its equivalent series resistance with frequency, such as achieved by some ferrite beads. Optimal resistance of either inductors or resistors will maintain loopgain margin at the desired operating frequency of the lamp, while reducing loopgain at other frequencies such that extraneous oscillations are prevented.

FIG. 55 provides another example embodiment schematic representation for the ballast electronics of the induction lamp in an implementation of the burst operational mode, where the timing circuit is configured to operate more efficiently in the ballast circuit by utilizing the inverter's start-up bias power. In this example embodiment, resistors R2, R3, and R7 in the oscillator serve to initiate the self-oscillation when power is first applied to the circuit by providing a positive gate-to-source voltage on transistor Q1, which allows current to flow through it. This current flow causes the switch node voltage to rise rapidly to VC+, initiating the inverter circuit oscillation. By connecting the positive supply voltage node (Vosc+) of the timing circuit to the switch node through diode D5, and the negative supply voltage node (Vosc−) in series with resistor R7, the current that normally flows through the start-up resistor R7 can also be used to bias the timing circuit. This eliminates the additional current draw of resistor R1 in the FIG. 53 embodiment. The timing circuit deactivates the inverter by turning on transistors Q7 and Q8, which force the gate-to-source voltages of inverter transistors Q1 and Q2 to zero volts. When the timing circuit turns off Q7 and Q8, the inverter resumes normal self-oscillating operation. In addition to requiring less additional ballast power to operate the timing circuit, this embodiment can offer faster and more consistent re-start of the inverter because of the preferred initial conditions set by transistors Q7 and Q8. As mentioned previously, Q7 and Q8 force zero volts gate-to-source on the inverter power transistors Q1 and Q2 in order to disable the inverter oscillation. When Q7 and Q8 turn off, the inverter is in a well-defined state from which it reactivates quickly and consistently.

FIGS. 56A-E provide alternate embodiment examples for implementing a timing circuit 5204. It is possible for the timing circuit 5204A to enter a stable non-oscillating state. This can occur if transistors Q3 and Q4 are both in the saturation condition in which base current flows into both devices and both base-to-collector voltages are positive at the same time. In this case, the capacitors C13 and C14 do not create the positive feedback loop that normally causes the circuit to oscillate. This condition can be prevented by adding some components to prevent transistors Q3 and Q4 from saturating, such as in the alternate timing circuits 5204B-F.

FIG. 57 provides an alternate embodiment example for implementing a charge pump to provide increased current to Vosc of the timing circuit 5204, such as if the current draw of the timing circuit from Vosc is high enough that supplying Vosc through R1 causes issues. Increased current can also be supplied to Vosc by a slightly more complicated charge pump circuit, shown below. In this example, the charge pump circuit operates in parallel with R1's linear supply, and relies on the movement of the switch node voltage while the inverter is enabled. When the switch node voltage makes its transition from VC+ to VC−, C2 is charged (VC2 is positive) through D3 and C1. This pushes current into C1 and Vosc, thereby supplying power to Vosc. When the switch node voltage makes the opposite transition, from VC− to VC+, C2 is discharged through D4 and the circuit is reset for the next transition. A larger value of C2 will allow more current to flow during the switch node transitions and supply a higher DC current to Vosc. C1 is especially important in this case to absorb the short pulses of current supplied through D3 and filter them into a steady DC value. A small-value resistor, R4, limits D3 and D4 current during edge-case transient conditions. It is important to note that the charge pump circuit will only supply current to Vosc while the inverter is enabled; while the inverter is disabled, only R1 supplies current to Vosc. A sufficiently large value for C1 will filter out this variation in supply current.

FIG. 58 provides an embodiment example for implementing a fast turn-on circuit. When the timing circuit 5204 enables the inverter 5208 by turning off Q5 of the circuit 5206, the inverter's re-start process is controlled by R2, R3, Cg, and Cfbk (such as depicted in FIG. 53). When Q5 turns off, the gate-to-source voltage of Q1 and Q2 (“inverter Vgs”) is initially at almost 0V. R2 slowly charges up the combination of Cg and Cfbk from VC+, with R3 slightly counteracting the charging by diverting some of the charging current; when the inverter Vgs reaches Q1's Vgs-threshold voltage, Q1 turns on and the self-oscillation begins. This delay between Q5 turning off and the inverter restarting decreases the effective duty cycle of the light output. With realistic component values, the delay may be long enough that it can significantly impact the light output duty cycle at the optimal modulation frequencies (e.g., 1 kHz and above). Besides decreasing the maximum possible duty cycle, this re-start delay may also add significant manufacturing variation, as it is heavily dependent on Q1's Vgs-threshold voltage, which varies widely between individual devices and over temperature. To reduce this delay, the fast turn-on circuit depicted in FIG. 53 may be added, consisting of Q6, R6, R5, and C3. When Q4's collector voltage is at Vosc and Q5 is enabled, R5 keeps Q6's gate-to-source voltage at 0V and Q6 is off. When Q4's collector voltage goes to 0V, disabling Q5, the rapid voltage transition applies a short negative pulse to Q6's gate through C3, and Q6 turns on for a short time before R5 returns its gate-to-source voltage to 0V again. During the short time in which Q6 is on, Vosc rapidly charges up Cg and Cfbk through R6, accelerating the inverter re-start process. R6's value is large enough that it doesn't affect the inverter's operation while the inverter is running and Q6 is off.

An example RF fluorescent lamp includes a bulbous vitreous portion of the RF fluorescent lamp comprising a vitreous envelope filled with a working gas mixture; a power coupler comprising at least one winding of an electrical conductor for receiving an alternating voltage and current to generate an alternating magnetic field and thereby induce an alternating electric field within the vitreous envelope, the at least one winding having a first end and second end, the first end receiving the alternating voltage and current and the second end connected to local ground; and an electronic ballast providing appropriate voltage and current to the first end of the winding of the power coupler, the voltage and current provided with reference to local ground, wherein the electronic ballast comprises an inverter circuit operating at a first frequency that provides the voltage and current with reference to local ground to a switching node connected to the first end of the winding of the power coupler, a timing circuit operating at a second frequency equal to or less than half the first frequency, and an enable circuit activated by the timing circuit that enables and disables the inverter circuit.

One or more certain further aspects of the example RF induction lamp may be incorporated in certain embodiments. The timing circuit may periodically enable the inverter to produce a burst-mode operation of the RF fluorescent lamp at the second frequency such that the voltage and current is enabled and provided to the power coupler for a first period and disabled for a second period. The second period may be short enough that the working gas mixture does not have enough time to dissipate completely after having been previously energized. The timing circuit may be adapted to decrease the rise-time associated with the onset of the first period by a fast turn-on circuit. The power coupler may include a high-Q coupler core. The high-Q coupler may enable elevated coupler voltage amplitude for shorter time durations to improve lamp energy efficiency. The timing circuit is a floating oscillator circuit operating with reference to the switching node of the inverter circuit.

In embodiments, a high-Q power coupler core may be utilized to improve efficiency through fast re-strike, such as illustrated in FIG. 59. Each time the inverter 5208 re-starts, to begin producing light it must re-form the plasma inside the burner by creating a high AC voltage on the coupler (that is, the “strike”). The off-times are short enough that the plasma doesn't have enough time to dissipate completely while the inverter is disabled, and these “repetitive strikes” require less time and energy than the very first strike event when the lamp is first turned on. The energy consumed by the repetitive strikes still has an impact on lamp efficiency, however, as they consume energy but produce little light. The length of time required for each strike is inversely proportional to the coupler voltage amplitude, thus, higher strike voltages result in a faster strike, and vice versa. The attainable coupler voltage depends on the losses in the ballast's resonant circuit, where lower losses lead to less damping in the resonant circuit and create a higher strike voltage. Higher strike voltages consume more instantaneous power, but because of the reduced strike time result in lower overall strike energy. Therefore, to improve efficiency a power coupler may be used with a core material which has low losses at the operating frequency, such as at 2-3 Mhz. As the power coupler is part of the ballast's resonant circuit this allows higher strike voltages, and consequently reduces repetitive strike time and increases efficiency.

While only a few embodiments of the present invention have been shown and described, it will be obvious to those skilled in the art that many changes and modifications may be made thereunto without departing from the spirit and scope of the present disclosure as described in the following claims. All patent applications and patents, both foreign and domestic, and all other publications referenced herein are incorporated herein in their entireties to the full extent permitted by law.

All documents referenced herein are hereby incorporated by reference.

Claims

1. An RF fluorescent lamp, comprising: a bulbous vitreous portion of the RF fluorescent lamp comprising a vitreous envelope filled with a working gas mixture;a power coupler comprising at least one winding of an electrical conductor for receiving an alternating voltage and current to generate an alternating magnetic field and thereby induce an alternating electric field within the vitreous envelope, the at least one winding having a first end and second end, the first end receiving the alternating voltage and current and the second end connected to local ground; andan electronic ballast providing appropriate voltage and current to the first end of the at least one winding of the power coupler, the voltage and current provided with reference to local ground,wherein the electronic ballast comprises an inverter circuit operating at a first frequency that provides the voltage and current with reference to local ground to a switching node connected to the first end of the at least one winding of the power coupler, a timing circuit operating at a second frequency equal to or less than half the first frequency, and an enable circuit activated by the timing circuit that enables and disables the inverter circuit.

2. The RF fluorescent lamp of claim 1, wherein the timing circuit periodically enables the inverter circuit to produce a burst-mode operation of the RF fluorescent lamp at the second frequency such that the voltage and current is enabled and provided to the power coupler for a first period and disabled for a second period.

3. The RF fluorescent lamp of claim 2, wherein the second period is short enough that the working gas mixture does not have enough time to dissipate completely after having been previously energized.

4. The RF fluorescent lamp of claim 2, wherein the timing circuit is adapted to decrease a rise-time associated with the onset of the first period by a fast turn-on circuit.

5. The RF fluorescent lamp of claim 1, wherein the power coupler comprises a high-Q coupler core.

6. The RF fluorescent lamp of claim 5, wherein the high-Q coupler core enables elevated coupler voltage amplitude for shorter time durations to improve lamp energy efficiency.

7. The RF fluorescent lamp of claim 1, wherein the timing circuit is a floating oscillator circuit operating with reference to the switching node of the inverter circuit.

8. The RF fluorescent lamp of claim 1, wherein the bulbous vitreous portion of the RF fluorescent lamp comprises a remote glass sealing configuration.

9. The RF fluorescent lamp of claim 1, wherein the RF fluorescent lamp has an outward appearance of a G25 incandescent bulb.

10. The RF fluorescent lamp of claim 1, wherein the RF fluorescent lamp further comprises ballast electronics with layered EMI shielding and head spreader.

11. The RF fluorescent lamp of claim 1, wherein the RF fluorescent lamp utilizes UV light sources to excite a phosphor coating on the bulbous vitreous portion of the RF fluorescent lamp through at least one of non-mercury plasma discharge, UV light emitting diodes (LEDs), cathode ray tube emission, field-emission cathodoluminescence UV, and visible light generators.

12. The RF fluorescent lamp of claim 1, wherein the RF fluorescent lamp utilizes a first and second burner to provide temperature selection.

13. The RF fluorescent lamp of claim 1, further comprising a first coating deposited on the inner surface of the bulbous vitreous portion, the first coating comprising a first metal oxide; a second coating deposited on top of the first coating, the second coating comprising a phosphor; and a third coating deposited on top of the second coating, the third coating comprising a second metal oxide.