The present invention generally relates to optical displays, and more particularly relates to lamp drivers in optical displays.
Various types of optical displays are commonly used in a wide variety of applications including computer displays, televisions, cockpit avionics, night vision (NVIS) applications and the like. Included among these various types of optical displays are liquid crystal displays (LCDs) such as active matrix LCDs (AMLCDs). LCDs typically use a passive or active matrix display grid to form an image on the display surface. Such displays typically include any number of pixels on the display grid that are arrayed in front of a backlight. By controlling the light passing from the backlight through each pixel, color or monochrome images can be produced in a manner that is relatively efficient in terms of physical space and electrical power consumption.
Frequently, LCD backlights are implemented with fluorescent lamps or the like. A fluorescent lamp is any light source in which a fluorescent material transforms ultraviolet or other energy into visible light. Typically, a fluorescent lamp includes a glass tube that is filled with argon or other inert gas, along with mercury vapor or the like. When an electrical current is provided to the contents of the tube, the resulting arc causes the mercury gas within the tube to emit ultraviolet radiation, which in turn excites phosphors located inside the lamp wall to produce visible light. Fluorescent lamps have provided lighting for numerous home, business and industrial settings for many years.
Despite the widespread adoption of displays and other products that incorporate fluorescent light sources, however, designers continually aspire to improve the electrical efficiency of the light source, to extend the dimmable range of the light source, and/or to otherwise enhance the performance of the light source, as well as the overall performance of the display. In the avionics arena, in particular, there is a need to reduce power consumption while also improving the displayed image presented to the viewer across a wide range of luminance. Therefore, it is desirable to create an improved lamp driver system that provides a relatively wide luminance range and relatively precise brightness control while providing good electrical efficiency.
In various embodiments, a driver circuit provides electrical energy from a power source to a fluorescent lamp such as that used in a flat panel display, head-up display, liquid crystal display and/or the like. Power is provided to the lamp via a transformer with a primary and a secondary winding, with the ends of the secondary winding coupled to the fluorescent lamp. A high-side current steering circuit is configured to switchably provide a drive output coupling the power source to the transformer in response to a switch input. In various embodiments, a current control loop is configured to adjust the input to the high-side current steering circuit in response to the current in one of the windings of the transformer and/or a luminance control loop is configured to adjust the switch input in response to the brightness of the light. A lamp current frequency control loop may then be configured to adjust an electrical polarity of the primary winding to adjust the frequency of current applied to the lamp.
The present invention will hereinafter be described in conjunction with the following drawing figures, wherein like numerals denote like elements, and
The following detailed description of the invention is merely exemplary in nature and is not intended to limit the invention or the application and uses of the invention. Furthermore, there is no intention to be bound by any theory presented in the preceding background of the invention or the following detailed description of the invention.
According to various exemplary embodiments, a lamp driver circuit with at least three resonant loops provides for highly efficient and effective lamp operation. A current control loop and a luminance control loop are provided, along with a separate lamp current frequency control loop that controls the frequency of electrical current applied to the lamp. This “frequency loop” obtains a trigger signal from the transformer coupled to the lamp, or from another source as appropriate. The trigger signal is then processed with suitable analog and/or digital circuitry to provide appropriate electrical signals coupled to each end of the primary transformer winding. By separating the polarity of the applied power from the current and luminance control loops, the frequency of the drive signal applied across the lamp can be increased or otherwise adjusted. These adjustments in frequency can improve the efficiency of the light source, reduce undesirable electromagnetic interference (EMI) emissions, and/or produce other benefits.
The term “coupled” in the context of this document refers to the direct or indirect connection of two devices or objects in a physical, logical, electrical or other appropriate sense. While devices “coupled” together may electrically communicate or otherwise interoperate with each other, they need not be physically joined together. In particular, two objects that are “coupled” together may have one or more intervening objects (e.g. electrical components such as resistors, capacitors, digital or analog filters and/or the like) between them and need not be in direct physical or electrical contact with each other.
Referring now to
The main arc drive circuitry 100 suitably includes at least a current control circuit 162 and an optical feedback circuit 164 that control lamp current and lamp luminance, respectively. As shown in
Source leads of the switches 108, 110 are shown connected together and through a current sense resistor 138 (e.g. a resistor of about 0.025-ohms or so) to signal return. Continuous current in sense resistor 138 is filtered and amplified in loop 162; this signal drives the positive input of a hysteretic comparator 134. The output of the hysteretic comparator in the
The two N-channel FET drivers 108 and 110 are driven by signal 135, which in this embodiment is shown to coincide with drive signal 101. Signal 135 is provided as a clock input to a D flip-flop with latching output. D flip-flop operation ensures only one N-channel FET is on at any time. In operation, the rising (or trailing) edge of any pulse arriving on signal line 135 can shift the signal 137 provided at the data (D) input of the device. In practice, signal 137 is provided from the inverting output (/Q) of the same device, thereby providing that switched 108 and 110 should remain in opposite (i.e. activated or non-activated) states, and that the states of each switch 108, 110 should change on any rising edge of signal 135. As noted below, this same structure can receive an input 135 from other sources in circuit 100 to improve operation. Signal 135 can be obtained from the power switch 106, from inductor 124, from transformer 120 and/or for any other signal node existing between the voltage source 102 and lamp 104 as appropriate. Since flip-flop 130 in this embodiment is toggled by any rising voltage edge on signal 135, many equivalent input signals 135 could be provided. Additionally, flip-flop 130 could be equivalently replaced with a trailing edge flip-flop, with a conventional latch circuit, with discrete components configured to provide latching functions, and/or with any other logical or electrical equivalent as appropriate.
Current control loop 162 regulates the flow of current through the plasma in the fluorescent lamp for a particular luminance desired to be produced from the lamp. The desired luminance is provided by an input drive signal 149 that is received from an external control source as appropriate. High-side current steering, controlled by a hysteretic comparator 134, maintains the level of current for the given light output by periodically or aperiodically refreshing the current control source (e.g. transformer 120) with power from power supply 102. Low-side current steering, also driven from the hysteretic comparator 134 in
Generated light suitably exits the lamp at an angle that may be approximately normal to the outside glass surface. Some of this light impinges on a photodiode, photosensor and/or other photon-to-current converter 144 that is coupled to the arc drive circuitry via optical feedback circuit 164. The optical feedback circuit 164 obtains an electrical signal from photon to current converter (e.g. photodetecting diode 144) that measures the luminous flux coming from the lamp 104, and that outputs a proportional electrical current. This current can then be converted to a voltage and provided to an input of an error amplifier 148 to produce an optical amplifier that has relatively high gain at low luminance and exponentially decreasing gain at high luminance. The logarithmic amplifier 146 helps control stability in the optical control loop when higher levels of luminance and power are desired from the fluorescent lamp driver 100. The error amplifier 148 in turn drives an input to the hysteretic converter 134 described above. Luminance command signals 149 to lamp driver 100 may be obtained and processed as appropriate.
The positive input terminal of the error amplifier 148 is generally maintained at or near zero (or some other reference) potential. The output of error amplifier 148 can be compared with the output of the current control loop amplifier 132 at hysteretic converter 134 as appropriate. This hybrid control arrangement causes the current control loop circuitry 162 to drive plasma in the fluorescent lamp, thereby generating an intensity of fluorescent light corresponding to a signal out of the optical amplifier 146 that has the effect of negating luminance commanded signals 149. Hysteretic comparator 134 thus couples the current control loop 162 with the optical feedback loop 164, and it is the complex interplay between the two loops and the fluorescent lamp, which determine the physical processes occurring with plasma in the lamp channel.
The effects of current control loop 162 and luminance control loop 164 therefore combine to produce a resonant drive signal 125 to transformer 120, which in turn provides a drive signal to lamp 104 that is determined as a function of drive signal 125 and the polarity of winding 126, which in turn is determined by the conducting or non-conducting states of switches 108 and 110. In the embodiment shown in
Filter 203 processes the received signal 202 by applying any suitable delay or other filter to produce an output with desired timing characteristics. Filter 203 may also incorporate a low or band pass filter to remove high-frequency noise from (at least) the edges of the input signal to produce an output signal 135 having a desired waveform and frequency. In various embodiments, filter 203 is an active filter that adjusts the frequency of signals 135 in response to the intensity of light produced by lamp 104; this may be accomplished by adjusting filter 203 in response to an output 209 from optical control circuit 164 or error amplifier 148. In other embodiments, however, filter 203 is a more passive filter that does not obtain input from the light intensity loop, and signal 209 is omitted. Filter 203 may also incorporate an amplifier (e.g. one or more operational amplifiers) to amplify and/or attenuate input signals 202 as appropriate.
Rectifier/limiter 201 is any circuit or the like capable of further shaping signals 202. Signals 202 may be rectified using a conventional diode rectifier, for example. The rectified signals may be further limited at any appropriate voltage to prevent overloading of amplifier 204 or other circuitry. In various equivalent embodiments, rectifier circuit 201 is eliminated, placed in front of filter 203, incorporated within filter 203 and/or otherwise located within loop 205.
Amplifier 204 is provided in any appropriate manner; in various embodiments, amplifier 204 is effectively a digital amplifier that provides a high or low reference (e.g. “rail”) voltage at the output in response to input signals. This digital-type output can be useful in providing a sharp clock signal to flip-flop 130 in some embodiments. Alternatively, filter 203 could incorporate any sort of analog amplifier as appropriate to equivalently encompass the function of amplifier 204.
In many embodiments, it may be desirable to toggle the polarity of winding 126 at a rate that is relatively fast with respect to the rate at which signal 125 changes. This rate can be determined using conventional RC filter design techniques. Moreover, conventional low, band and/or high-pass filtering techniques using RC or other analog filtering components can be used to shape the edges of signal 202 as desired. In alternate embodiments, digital sampling and filtering techniques can be used. One or more amplifiers 104 (which may be an op amp or other amplification module) can also be provided to amplify and/or attenuate signals 202 so that they produce signals of 135 with appropriate magnitude for flip-flop 130. As noted above, the signals 135 are generally provided to the “clock” input of flip-flop 130, which suitably responds to rising and/or falling edges of signals 135 to toggle the outputs provided at the “Q” and “/Q” terminals of the device.
Various embodiments of loop driver circuitry 100 therefore provide a drive control loop 205 that operates at a different rate from the signal 101 produced by current loop 162 and/or optical control loop 164. Because the polarity of the voltage applied across winding 126 can be separated from the drive signal 125 itself in this manner, high frequency AC drive signals can be applied to lamp 104, and/or performance of circuit 100 may be improved as appropriate. This adjustment in AC frequency may also be used to avoid undesirable RF emissions at particular frequencies (e.g. at a frequency that interferes with another component in a display system), or for any other purpose.
The concepts set forth above are generally referenced in the context of a “triple loop” driver circuit having a current control loop, a light intensity control loop and a drive control loop for ease of understanding. In practice, however, the concepts of a drive control loop may be implemented distinct from the current control and/or light intensity loops across a wide variety of alternate, yet equivalent, embodiments.
While at least one exemplary embodiment has been presented in the foregoing detailed description of the invention, it should be appreciated that a vast number of variations exist. It should also be appreciated that the exemplary embodiment or exemplary embodiments are only examples, and are not intended to limit the scope, applicability, or configuration of the invention in any way. Various changes may be made in the function and arrangement of elements described in the exemplary embodiments without departing from the scope of the invention as set forth in the appended claims and their legal equivalents.
This is a continuation-in-part of application Ser. No. 10/788,895 entitled “Fluorescent Lamp Driver System” filed Feb. 27, 2004.
Number | Date | Country | |
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Parent | 10788895 | Feb 2004 | US |
Child | 11695216 | Apr 2007 | US |