The invention relates to a method for driving gas discharge lamps as described in the preamble of claim 1. The invention also relates to a circuit for driving gas discharge lamps as described in the preamble of claim 4.
U.S. Pat. No. 6,023,131 discloses a backlight device for a liquid crystal display (LCD), which comprises a high-voltage generating means, whose output can be controlled. The high-voltage generating means comprises an inverter for generating an alternating output voltage. The output of the inverter is connected to first electrodes of three gas discharge lamps, which can emit red, green and blue light, respectively. A second electrode of each lamp is connected to a ground voltage line via a separate first electronic switch. The inverter is connected to a high-voltage source via a second electronic switch. A control circuit is connected to the switches to let them conduct or to block. Only when the second switch is conducting the high voltage is supplied to the inverter, so that it will generate the alternating voltage. The three first switches are controlled such that only one first switch is conducting at a time. There is an off-interval of not conducting of all first switches between on-times of different first switches being conducting. Only the selected one lamp will emit light.
With said prior art backlight device each lamp may emit light during a small part, in particular less than one third, of time only. Therefore, to obtain a certain amount of light during some time on average a relatively high peak current must flow through the lamps. Therefore also, the inverter, the switches and the lamps must be suitable to handle such high peak currents, which causes them to be relatively bulky and expensive.
An object of the invention is to solve the drawbacks of the prior art method and circuit as described above.
The above object of the invention is achieved by providing a method for driving gas discharge lamps as described in claim 1. Accordingly, each lamp can be controlled to emit light or not individually for all of the time, and in practice from 1% to 100% of the time. Therefore, peak intensities and peak currents may be lower than before for obtaining the same average intensity during some time, so that the circuit and the lamps need to be less powerful and less expensive.
The above object of the invention is achieved also by providing a circuit for driving gas discharge lamps as described in claim 4.
The invention will become more gradually apparent from the following exemplary description in connection with the accompanying drawing. In the drawing:
The circuit diagram shown in
Although in here an example using three lamps 2 is described, the invention is applicable for any number of lamps 2, each emitting light of any part of the spectrum.
Each lamp 2 (2a, 2b, 2c) has a first electrode 4 (4a, 4b, 4c, respectively) and a second electrode 6 (6a, 6b, 6c, respectively). The electrodes 4 and 6 may be of a type which are heated by heating means to promote ignition of the lamps 2. For simplicity of the drawings and the description such heating means are not shown and are not described in detail in here.
The circuit of
During operation the frequency controller 12 compares a reference voltage (not shown) with a voltage received from the voltage sense circuit 14 to provide an error voltage. The frequency controller comprises a voltage controlled oscillator (VCO, not shown) which generates a rectangular voltage of which the frequency is dependent on said error signal. Said rectangular voltage is supplied to the inverter controller 10. The inverter controller 10 comprises level shifters (not shown) to supply complementary control signals to control inputs (gates) of the half-bridge switches 18 and 20, so that they are switched on and off alternately and a rectangular high voltage is generated at the connection node of said switches 18 and 20 and inductor 22. The resonant circuit of inductor 22 and capacitor 24 is designed to resonate on a resonance frequency which is basically the same as the frequency of the rectangular voltage at the connection node of the half-bridge switches 18 and 20. As a result, a basically sinusoidal voltage will be generated at the connection node of inductor 18 and capacitor 24 of the resonant circuit.
The power controller 16 is connected to control inputs (gates) of the electronic switches 28, called lamp switch hereinafter. The power controller 16 may receive data from some exterior data source (not shown) by which the power controller may control the lamp switches 28. If a lamp switch 28 is conducting an alternating current may flow through the lamp 2 connected in series with that lamp switch 28. By providing appropriate data to the power controller 16 and, accordingly, appropriate pulse widths of control signals to the lamp switches 28 any light color within the gamut of the lamps 2 can be obtained.
The power controller 16 may control the lamp switches 28a, 28b, 28c to conduct or to block individually, that is, to conduct or to block at any time and at the same time with other ones of the lamp switches 28. That poses a problem for controlling the light intensities (or lamp power) provided by the lamps 2 as will be explained now.
A gas discharge lamp 2 almost behaves like a constant voltage source, that is, a lamp voltage (across the lamp only) is almost constant. Suppose one wants to keep the light emission power of the lamp 2 constant. One could measure a current through a lamp 2 and control it to keep it constant. With the lamp voltage being constant the light emission power will be kept constant then. A current trough a lamp 2 can be changed by changing the impedance of the capacitor 26 in series with the lamp 2, that is, by changing the frequency of the current. However, said frequency applies for all series circuits of a lamp 2 and a capacitor 26. Therefore, controlling the frequency for keeping a current through one lamp 2 constant will influence a current through an other lamp 2, so that a voltage across the series circuits changes, the frequency is changed to keep the current in said other lamp 2 constant, with the result that the current through the first mentioned lamp 2 changes, which needs control to keep it constant, and so on, so that the control of lamp currents may become unstable and light flicker may occur.
If one wanted to control a total current flowing through the total load of conducting lamps 2, instead of controlling currents through individual lamps 2, some additional series load would be required to measure the total current. That would mean loss of energy. Also, at any time one should know which or how many lamps 2 are conducting to determine a reference or goal value for the total current. This is not practical.
According to the invention, in parallel to the total load represented by the lamps 2 there is connected a filter having an impedance and response characteristic which are identical (in theory) to the impedance and response characteristic provided by a lamp 2 and the stabilizing capacitor 26 in series therewith. As shown in
C30·R32=C26·Rlamp (1)
wherein:
C30 is the value of capacitor 30,
R32 is the value of resistor 32,
C26 is the value of a stabilizing capacitor 26, and
Rlamp is the resistance value of a lamp 2 on average when conducting.
With such a filter 30, 32, a node thereof will have a voltage which is proportional to a voltage at a node of a series circuit of a lamp 2 and a capacitor 26 for all values of the frequency of the current supplied to the lamps 2. When the frequency changes, as explained below by control, the impedance of the capacitors 26 changes, so that a voltage across the series circuits of a lamp 2 and a capacitor 26 and the filter 30, 32 changes. With the lamps 2 and capacitors 26 being substantially identical all individual lamp currents are in phase, so that their influence on a control of the frequency will be identical and a stable control can be provided.
The voltage sense circuit 14 is supplied with an alternating voltage appearing at the node of capacitor 30 and resistor 32 of the filter. The voltage sense circuit 14 determines a value of a property of said voltage, such as a root mean square (RMS) value, which can be used as feed back signal value in control loop, comprising the frequency controller 12 also, to control the power of the lamps 2.
It is observed that the lamps of a lighting system, such as a backlight device, may have different resistance values when conducting. At the time of manufacturing, lamps of the same type may have a resistance value distribution of up to +/−10%. Such a variation may be compensated for by inserting a resistor in series with the lamp and possibly by adjusting such resistor to meet the above condition (1). In practice, applying the mean value of said distribution will be suitable to meet the above condition (1) and to achieve the wanted frequency and power compensations without using an additional component in series with each lamp.
Numerical example values are:
the high DC input voltage (V+ minus V−) may be 300V;
the voltage at the first electrodes 4 of the lamps 2 may be 400 Vrms;
the frequency of the lamp current may be 20 to 200 kHz;
the control signal to a lamp switch 28 may have a repetition frequency of 75 to 150 Hz.
More preferably, the over-voltage protection means comprises for each lamp switch 28 (28a, 28b, 28c) a resistor 38 (38a, 38b, 38c, respectively), which is connected in parallel to the corresponding diode 36 (36a, 36b, 36c, respectively). With the lamp switches 28 being deselected, the resistors 38 keep the drain voltage of the lamp switches 28 near the high DC voltage at line V+. In this way the parasitic drain-source capacitance of the MOSFET switches 28 is minimized. Such a resistor 38 may have a high value of, for example 100 kOhm to 1 Mohm.
Still more preferably, the over-voltage protection means may comprise also a zener diode (not shown) which is connected in series with said diode 36. In the example of
Number | Date | Country | Kind |
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05109989 | Oct 2005 | EP | regional |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/IB2006/053870 | 10/20/2006 | WO | 00 | 4/22/2008 |
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WO2007/049205 | 5/3/2007 | WO | A |
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