This disclosure relates to high intensity discharge lamps, and in particular, to ignition aids used in such lamps.
Differences exist in speed of breakdown and the number of electrons needed to initiate a self-sustained discharge, but the underlying breakdown mechanism is the same for low pressure discharges (e.g., fluorescent lamps) or high pressure discharges (arc discharge lamps). Discharge is initiated between two conductors that are given opposite electric potential. The space between the conductors usually comprises a gas, and efforts are made to maintain the quality/purity of the gas by enclosing it in a hermetic vessel. The essential end result of the discharge is the creation of a plasma between the two conductors. Plasma is defined as a conductive medium, containing equal proportions of electron and ions, which allows for conduction of electric current through an otherwise insulator material, i.e., the gas in its initial state.
Initially, the gas contained in the arc tube is non-conductive. If an electric potential is applied on the conductors, this creates a favorable situation to strip the outer orbital electrons from the atoms of the gas and thus create free electrons, which are then accelerated though the gas by the electric field generated between the conductors, and initiates more electrons by collision with gas atoms, which in turn are ionized. If the electric field is high enough, each electron thus created will create additional electrons by inelastic collisions with gas atoms and ions, and initiates an electron avalanche. Such an avalanche creates the discharge. However, to create such electrons by simple dielectric breakdown of the gas atoms by the electric field requires several kilovolts of electric potential. Higher and higher electric potentials require more expensive external electrical circuitry, and may not be commercially feasible. Unwanted breakdown can also occur in the outer jacket and in the cap-base region.
Discharges for commercial applications employ an additional source of free electrons, which removes the need for generating such high voltages to initiate the discharge. Such external sources can be a heated filament, use of the ever present cosmic rays, or providing a source of electrons by radioactive decay. Heated filaments are not practical in high intensity discharge (HID) lamps, and the cosmic ray background radiation is insufficient to dramatically reduce the need for very high electric fields needed to initiate the ignition, unless other methods are used to lower the breakdown voltage.
For providing a source of electrons by radioactive decay, typically what has been used in the past in the HID arc tube is a radioactive gas, such as Kr85 with most of the decay products being beta particles (i.e., electrons). Kr85 has a half-life of 10.8 years, with 99.6% of the decay products being beta particles (i.e., electrons) having a maximum kinetic energy of 687 kev. These electrons have very high energy, and in many respects are an ideal source for free electrons and used widely as such for these applications. But to provide enough of these high energy electrons by radioactive decay, significant quantity of this gas has been used in HID lamps.
The presence of Kr85 in such lamps diminishes the need for providing very high electric potential on the conductors, which makes the external electrical circuitry (a ballast) and systems design simpler and more cost effective. Typical applications use such a radioactive gas with a ballast that provides a high electric pulse for a very short duration, typically in the millisecond (microsecond) range, that is very effective in creating the electron avalanche referred to earlier. However, recent UN2911 government regulations limit the amount of radioactive Kr85 used in lamps. These regulations proscribe the HID lamp manufacturers from using the large quantity of Kr85 gas that has been previously used, as described in preceding paragraph.
A number of ignition aids have been designed for improving the ignition of high intensity discharge lamps. U.S. Patent application Pub. No. 2002/0185973 discloses a lamp in which wire is wrapped around both legs of the arc tube and its central body as both an ignition aid and for containment, but are not connected to the electrodes. Another reference, U.S. Pat. No. 5,541,480, discloses an ignition aid in which a conductor that is coated on an exterior surface of an arc tube of constant diameter between the electrodes is connected to a conductive frame wire that contacts an electrode. U.S. Pat. No. 6,222,320 discloses an ignition aid for a lamp including an arc tube having a central body portion and smaller diameter legs extending from the body portion, wherein a conductor that is in contact with a conductive frame wire that contacts one of the electrodes, contacts only the central body portion of the arc tube.
A need to reduce the Kr85 content in HID lamps exists, but such reduction could have serious consequence to discharge initiation, and consequently unacceptable performance. This invention describes a means to obviate this disadvantage of lowering the Kr85 gas content.
In one embodiment of this disclosure, a high intensity discharge lamp includes an electrically insulating arc tube including light transmissive material having a central portion and two legs each of which extends from the central portion. The central portion forms an interior discharge region in which an ionizable material is sealed therein. Electrical conductors each extend through one of the legs and are spaced apart from each other in the discharge region. A sealed shroud including light transmissive material encloses the arc tube and there is electrical connection to the electrical conductors through the sealed shroud. An electrically conductive frame member is disposed in an interior of the shroud and is electrically connected to one of the electrical conductors. An ignition aid including electrically conductive foil is fastened to the frame member and forms a closed loop that encircles one of the legs of the arc tube around one of the electrical conductors. The foil is insulated from the adjacent electrical conductor. The foil encircles the leg by an angle in a range of at least 270 degrees to 360 degrees. The foil includes two end portions, and a central portion therebetween that encircles the arc tube leg. A first end portion of the foil is connected to the frame member and a second end portion of the foil is connected to the foil between the central portion and the first end portion of the foil.
Referring to the following specific aspects of the high intensity discharge lamp of this disclosure, which can be used alone or in any combination in all embodiments disclosed herein, the legs and central body portion of the arc tube may have a circular cross-sectional shape. The legs are smaller in diameter than the arc tube. The foil can encircle the leg by the range of at least 300 degrees to 360 degrees, and in particular, by the range of at least 320 degrees to 360 degrees. There is no electrical conductor encircling an exterior surface of the other arc tube leg (the leg that is not in contact with the foil) or disposed on an exterior surface of the central portion of the arc tube. A width of the foil ranges from 1.0 mm to 4.0 mm and, more specifically, from 1.0 mm to 3.0 mm, in particular from 1.0 mm to 2.0 mm. A thickness of the foil is less than 0.2 mm, more specifically ranging from 0.01 mm to 0.15 mm, in particular in a range of 0.01 mm to 0.08 mm and specifically can be 0.076 mm. A ratio of a width of the foil to a thickness of the foil ranges from 6.6:1 to 400:1. Each of the legs of the arc tube can include a flange and a boss extending from the flange into the discharge region so that the flange abuts the central portion. The central portion can be a cylindrical barrel. A distance from an outer surface of the flange to a proximal edge of the foil is not more than 8.0 mm and, in particular, not more than 2.0 mm.
The arc tube can include polycrystalline alumina. The discharge region can be filled with inert gas (e.g., argon gas), krypton gas and a dose of mercury and metal halides. A mixture of argon gas and Kr85 gas present in the discharge region can have an activity concentration of not greater than 0.16 MBq/liter. The arc tube can be at a pressure of 100-500 millibar. The electrical conductors can include a first conductor to which voltage is applied and a second conductor spaced apart from the first conductor in the arc tube, wherein the frame member is electrically connected to the second conductor (and does not connect with the first conductor) and the foil is wrapped around the leg around the first conductor. The first end portion of the foil can be connected to the frame member, and the second end portion of the foil can be connected to the foil, by welding. The foil can be comprised of a base metal selected from the group consisting of Nb, Mo, Ta, Pt, Re, W, Ni, and combinations thereof, and a combination of any of the base metals with cladding comprised of one or more of the base metals.
A second embodiment of the disclosure features a high intensity discharge lamp. An electrically insulating arc tube comprised of light transmissive material has a central portion and two legs each of which extends from the central portion. The central portion forms an interior discharge region. Each of the legs includes a flange and a boss extending from the flange into the discharge region so that the flange abuts the central portion. Electrical conductors each extend through one of the legs and are spaced apart from each other in the discharge region. A sealed shroud comprised of light transmissive material encloses the arc tube and there is electrical connection to the electrical conductors through the sealed shroud. An electrically conductive frame member disposed in an interior of the shroud is electrically connected to one of the electrical conductors. An ignition aid comprises electrically conductive foil that is fastened to the frame member and forms a closed loop that encircles one of the legs of the arc tube around one of-the electrical conductors. The foil encircles the leg by an angle in a range of at least 270 degrees to 360 degrees. A distance from an outer surface of the flange to a proximal edge of the foil ranges from 1.5 to 8 mm.
As to specific features of the lamp of the second embodiment, a thickness of the foil can range from 0.01 mm to 0.15 mm. A width of the foil can range from 1 mm to 4 mm. A mixture of argon gas and Kr85 gas present in the discharge region can have an activity concentration of not greater than 0.16 MBq/liter. Any of the specific features discussed in connection with the lamp of the first embodiment can also be used in the lamp of the second embodiment.
A third embodiment of the disclosure features a high intensity discharge lamp that includes an electrically insulating arc tube including light transmissive material having a central portion and two legs each of which extends from the central portion. The central portion forms an interior discharge region in which an ionizable material is sealed therein. Electrical conductors each extend through one of the legs and are spaced apart from each other in the discharge region. A sealed shroud including light transmissive material encloses the arc tube and there is electrical connection to the electrical conductors through the sealed shroud. An electrically conductive frame member is disposed in an interior of the shroud and is electrically connected to one of the electrical conductors. An ignition aid including electrically conductive foil is fastened to the frame member and forms a closed loop that encircles one of the legs of the arc tube around one of the electrical conductors. The foil is insulated from the adjacent electrical conductor. The foil encircles the leg by an angle in a range of at least 270 degrees to 360 degrees. A width of the foil ranges from 1 mm to 4 mm.
Referring to specific aspects of the third embodiment, each of the legs can include a flange and a boss extending from the flange into the discharge region so that the flange abuts the central portion. A distance from an outer surface of the flange to a proximal edge of the foil ranges from 1.5 to 8 mm. A thickness of the foil ranges from 0.01 mm to 0.15 mm. A mixture of argon gas and Kr85 gas present in the discharge region can have an activity concentration of not greater than 0.16 MBq/liter. Any of the specific features discussed in connection with the lamp of the first embodiment can also be used in the lamp of the third embodiment.
The high intensity discharge lamps of this disclosure advantageously exhibit good ignition even when using low amounts of Kr85 gas, which limits the availability of free electrons by radioactive decay. In particular, a mixture of argon gas and Kr85 gas present in the discharge region can have an activity concentration of not greater than 0.16 MBq/liter. Particular features of the foil ignition aid of the high intensity discharge lamps of this disclosure, including foil width, foil wrapping angle around the arc tube leg and spacing of the foil away from the central portion of the arc tube, have been determined in this disclosure to lead to increasing Emax or the maximum electric field at the tip of the electrode, and results in improved ignition of the lamp even though low Kr85 gas is used.
It should be appreciated that terms such as upper, lower, top, bottom, right, left, and the like are relative terms that will change with the orientation of the lamp. These terms are used for improving understanding in this disclosure and should not be used to limit the invention as defined in the claims.
Many additional features, advantages and a fuller understanding of the invention will be had from the accompanying drawings and the Detailed Description of the Invention that follows. It should be understood that the above Brief Description of the Invention describes the invention in broad terms while the following Detailed Description of the Invention describes the invention more narrowly and presents embodiments that should not be construed as necessary limitations of the broad invention as defined in the claims.
Referring to
Referring to
Referring to
Into the discharge region 48 is charged an ionizable material including an inert gas (e.g., argon), metal halide and mercury. Krypton 85 (Kr85) gas may also be used in the discharge region in amounts reduced to comply with government regulations; for example, a mixture of argon gas and Kr85 gas present in the discharge region can have an activity concentration of not greater than 0.16 MBq/liter. The composition of the gas in the arc tube at room temperature is argon and krypton with some mercury. The dose in the lamp, for example, can include 5.7 mg of Hg and the following (weight %) metal halides: 51.2% NaI, 6.8% TlI, 16.6% LaI3 and 25.4% CaI2. The total dose weight of these halides can be 12 mg.
Electrical current supplied to the contacts reaches the electrodes via the frame members and feedthroughs, and generates an arc between the electrodes. One electrode (e.g., the electrode connected to feedthrough 28 in
A foil ignition aid is used to improve ignition of the lamp. The ignition aid includes electrically conductive foil (26, 104) that is fastened to the frame member (18, 89) and encircles a leg of the arc tube around a feedthrough extending in that leg. The foil is spaced apart and electrically insulated from the feedthrough it encircles by the electrically insulating ceramic material of the arc tube leg. While not wanting to be bound by theory it is believed that the foil (26, 104) functions as a capacitor. There is no electrical conductor encircling the arc tube leg opposite the foil ignition aid or at the central portion of the arc tube. For example, turning to
Referring to
The measurement of the wrapping angle, ψ (Phi), by which the foil encircles the arc tube leg can be seen in
Viewing from an end of the arc tube leg in
A width, w, of the foil ranges from 1.0 mm to 4.0 mm and, more specifically, ranges from 1.0 mm to 3.0 mm, in particular from 1.0 mm to 2.0 mm. A thickness of the foil is less than 0.2 mm, more specifically ranging from 0.01 mm to 0.15 mm, in particular in a range of 0.01 mm to 0.08 mm and specifically can be 0.076 mm. A ratio of a width of the foil to a thickness of the foil ranges from 6.6:1 to 400:1. The foil of this disclosure is different from a wire in terms of its geometry and electric field that can be generated. As width and thickness are the same for wire of a given diameter, the ratio of wire width to wire thickness is 1:1, much less than the foil width:foil thickness ratio of this disclosure.
The reason the foil is a further enhancement of the lamp starting phenomenon is described below. For purposes of explanation, a conventional discharge lamp does not have the foil starting aid, but contains Kr85 gas and Ar gas. A ballast is used to apply the high voltage transient pulse between the electrodes contained in the hermetically sealed discharge region of the arc tube. Relatively high concentrations of Kr85 gas that exceed current government regulations (e.g., 6.2 MBq/l) are used in the conventional discharge lamp to allow for the discharge to be initiated reliably over the rated life of such lamps. The electric field generated in the conventional discharge lamp is defined as the applied voltage/gap between the electrodes. The larger the gap between the electrodes, the lower the electric field. The lower the electric field, the harder it is to reliably initiate the discharge, even though Kr85 gas and the high voltage electric pulse that is provided by the ballast, are present. Referring to
The lamp of this disclosure will now be described by reference to the following examples, which present more specific information that should not be used to limit the invention as described by the claims.
This example describes data produced for ceramic metal halide discharge lamps using software by Comsol Multiphysics 2010 developed with the University of Budapest for electrostatic calculation using finite element analysis. Inputs into the software were parameters describing the geometry of the arc tube of the 39 W lamp shown in
Maxwell equations solved in the discharge geometry region by finite element analysis were as follows:
Gauss' law: ∇D=ρ,
Electric potential: E=−∇V;
Constitutive relation: D=∈0∈rE,
which above equations produce the following differential equation that was solved for V:
−∇(∈0∈r∇V)=0,
where V is the electric potential, ∈0 is the dielectric permittivity of a vacuum, ∈r is dielectric permittivity of the material in the given modeling space, ∇ is the directional derivative in the 3 directions of the Cartesian coordinate system (∂/∂x)/(∂/∂y)/(∂/∂z), and ρ is volume density of free charges.
The software ran the finite element analysis together with adaptive meshing using a variety of numerical solvers. The AC/DC module provides an environment for simulation of electromagnetic problems in 2 and 3 dimensions. The software used static modeling without moving charges. Electric field was measured using scalar values normalized at the tip of the powered electrode. The electrode proximal to the foil was treated as the powered electrode while the other electrode was at 0 potential. That unpowered electrode, the foil and the frame member were treated as grounded elements. The gas was given an ∈r value of 1, the ceramic was given an ∈r value of 10 and the vacuum space was given an ∈r value of 1.
Output of the software showing the effect of foil width on Emax was shown in
For all of the cold box measurements of this example, the requirements of ANSI:C78-389-2004-MOM were adhered to. Prior to cold box measurement, the lamps were aged for 30 minutes in position of measurement. If the lamps have been aged for regular photo interval on life test racks, there is no need to 30 minute aging, if the cold box is done first. Lamps were soaked for 6 hours at temperature in the cold box prior to measurement. Regarding lamp starting voltage requirements for lamps requiring auxiliary starting circuits, lamps shall start within the time specified at the ambient temperature indicated when the following sine wave open-circuit test voltages and a starting pulse at the minimum pulse characteristics described below are applied (Table 1). The characteristics are measured at the terminals of the lamp holder. The pulse is applied to the center terminal of the lamp base with the shell grounded.
Shown below are comparative testing for 39 watt ceramic metal halide lamps without foil and using argon and a higher level of Kr85 or using the foil aid of this disclosure (Design 1 of
It is seen that even with reduced Kr85 levels, the lamps perform exactly as the lamps with the higher Kr85 content. This would not be possible without the foil ignition aid of
The photometric results of this test shown below indicate that the foil did not have any deleterious effect on performance. LPW means lumens per watt; CCT means correlated color temperature and CRI means color rendering index.
The p-value in the above table is a statistical measure of whether the two populations are equivalent or different. A p-value of >0.05 implies that statistically, the same parameter from the two populations are identical.
Many modifications and variations of the invention will be apparent to those of ordinary skill in the art in light of the foregoing disclosure. Therefore, it is to be understood that, within the scope of the appended claims, the invention can be practiced otherwise than has been specifically shown and described.
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