JP6182863B2 - Discharge lamp lighting device, discharge lamp lighting method, and projector - Google Patents

Description

  The present invention relates to a discharge lamp lighting device, a discharge lamp lighting method, and a projector.

  Conventionally, discharge lamps (discharge lamps) such as ultra-high pressure mercury lamps, metal halide lamps, and xenon lamps have been used as light sources for projectors. In order to extend the life of such a discharge lamp, it is essential to reduce the load applied to the discharge lamp from start-up (dielectric breakdown) to steady lighting by arc discharge.

  One method of lighting the discharge lamp is a resonance method. In this resonance method, a high frequency voltage of about several tens of kHz is applied between a pair of electrodes of the discharge lamp using a resonance circuit (igniter) when starting the discharge lamp. After starting, the operation of lowering the driving frequency of the discharge lamp from the resonance frequency to a low frequency (about several hundred Hz) in steady lighting is performed.

  By the way, when the discharge lamp is turned on by the resonance method described above, a state (called half-wave discharge) in which the electrode on one side of the discharge lamp does not shift from glow discharge to arc discharge may occur when the discharge lamp is started. In this case, a spatter phenomenon due to glow discharge occurs and blackening occurs. Further, when the half-wave discharge is shifted to steady lighting, the discharge becomes unstable, and in some cases, the discharge lamp is extinguished. Further, tube wall discharge may occur in the discharge lamp during half-wave discharge. In such a case, the deterioration of the discharge lamp is accelerated.

  Therefore, it is desirable to eliminate such half-wave discharge as much as possible before shifting to steady lighting. For example, with regard to a method for eliminating half-wave discharge, it is proposed to provide a half-wave discharge detection unit for detecting half-wave discharge, and to perform a half-wave discharge improvement process based on the detection result by the half-wave discharge detection unit (See Patent Document 1). However, when such a function of detecting a half-wave discharge is added in the control unit, there is a drawback that it is costly.

  On the other hand, a method has been proposed in which half-wave discharge is eliminated by amplifying the current flowing through the discharge lamp while gradually decreasing the resonance frequency (see Patent Document 2). However, this method has a problem that acoustic resonance occurs in the discharge lamp when the drive frequency is reduced.

JP 2010-108658 A JP 2011-1119044 A

  The present invention has been proposed in view of such conventional circumstances, and a half-wave discharge generated in the discharge lamp from the start of the discharge lamp to the steady lighting is changed to a full-wave discharge. It is an object of the present invention to provide a discharge lamp lighting device and a discharge lamp lighting method that can be appropriately and easily shifted, and a projector including such a discharge lamp lighting device.

  In order to achieve the above object, a discharge lamp lighting device according to the present invention is a discharge lamp lighting device that controls lighting of a discharge lamp, and controls a driving unit that drives the discharge lamp and driving of the driving unit. And a control unit that, when the discharge lamp is started, the drive unit drives the discharge lamp at a resonance frequency, and after the start period, the drive unit drives the discharge lamp. The discharge by the drive unit between a rising period until the frequency is lowered to a steady frequency lower than the resonance frequency and a steady period in which the driving unit drives the discharge lamp at the steady frequency after the rising period. The driving of the lamp is controlled, and an amplification period for amplifying at least a driving current supplied from the driving unit to the discharge lamp is provided after the predetermined period in the starting period. And performing control.

  In this discharge lamp lighting device, a half-wave discharge generated in the discharge lamp is converted into a full-wave discharge by providing an amplification period for amplifying at least the drive current supplied from the drive unit to the discharge lamp after a predetermined period in the start-up period. Appropriate and easy migration is possible.

  The amplification period may be provided during a period from the middle to the end of the arc starting period from when the discharge lamp shifts from glow discharge to arc discharge until the starting period ends. preferable.

  In this case, the load applied to the discharge lamp can be reduced while appropriately and easily shifting the half wave discharge generated in the discharge lamp to the full wave discharge.

  Further, the control unit reduces the drive current supplied to the discharge lamp simultaneously with the start of the start-up period, and stepwise the drive current supplied to the discharge lamp until the end of the start-up period. Alternatively, it is preferable to perform control for continuous amplification.

  In this case, by reducing the drive current supplied to the discharge lamp simultaneously with the start of the start-up period, the load applied to the discharge lamp can be reduced even if tube wall discharge occurs in the discharge lamp. Can do. On the other hand, after the drive current is reduced, the drive current supplied to the discharge lamp is amplified stepwise or continuously until the end of the start-up period, thereby generating blackening due to the temperature drop in the discharge lamp. Can be suppressed.

  Further, it is preferable that the control unit divides the start-up period into a plurality of periods and performs control to lower the driving frequency of the discharge lamp for each period.

  In this case, it is possible to suppress a sudden change when the driving frequency of the discharge lamp is lowered from the resonance frequency in the starting period to the steady frequency in the stationary period, and to stably shift the discharge lamp to the steady lighting state.

  Further, the discharge lamp lighting method according to the present invention is a discharge lamp lighting method for controlling lighting of the discharge lamp, and a start period for driving the discharge lamp at a resonance frequency when starting the discharge lamp, and after the start period Including a rising period until the driving frequency of the discharge lamp is lowered to a steady frequency lower than the resonance frequency, and a steady period for driving the discharge lamp at the steady frequency after the rising period, and in the starting period, An amplification period for amplifying at least the drive current supplied to the discharge lamp is provided after a predetermined period.

  In this discharge lamp lighting method, a half-wave discharge generated in the discharge lamp is changed to a full-wave discharge by providing an amplification period for amplifying at least the drive current supplied from the drive unit to the discharge lamp after a predetermined period in the starting period. Appropriate and easy migration is possible.

  The amplification period is preferably provided during a period from the middle to the end of the arc starting period from when the discharge lamp shifts from glow discharge to arc discharge until the starting period ends.

  In this case, the load applied to the discharge lamp can be reduced while appropriately and easily shifting the half wave discharge generated in the discharge lamp to the full wave discharge.

  Further, the drive current supplied to the discharge lamp is reduced simultaneously with the start of the start-up period, and the drive current supplied to the discharge lamp is amplified stepwise or continuously until the end of the start-up period. It is preferable to make it.

  In this case, by reducing the drive current supplied to the discharge lamp simultaneously with the start of the start-up period, the load applied to the discharge lamp can be reduced even if tube wall discharge occurs in the discharge lamp. Can do. On the other hand, after the drive current is reduced, the drive current supplied to the discharge lamp is amplified stepwise or continuously until the end of the start-up period, thereby generating blackening due to the temperature drop in the discharge lamp. Can be suppressed.

  Further, it is preferable that the startup period is divided into a plurality of periods and the driving frequency of the discharge lamp is lowered for each period.

  In this case, it is possible to suppress a sudden change when the driving frequency of the discharge lamp is lowered from the resonance frequency in the starting period to the steady frequency in the stationary period, and to stably shift the discharge lamp to the steady lighting state.

  A projector according to the present invention includes any one of the above discharge lamp lighting devices.

  In this projector, by providing any one of the above-described discharge lamp lighting devices, it is possible to perform discharge lamp lighting control with excellent reliability, and it is possible to extend the life and improve the quality of the discharge lamp.

It is a block diagram which shows the example of 1 structure of the projector by this embodiment. It is a block diagram which shows the example of 1 structure of the discharge lamp lighting device by this embodiment. It is an example of the waveform figure in the starting period of the drive current for demonstrating lighting control (discharge lamp lighting method) of the discharge lamp lighting device by this embodiment. It is an example of the waveform diagram in the rising period of the drive current by the lighting control of the present invention. It is an example of the waveform diagram in the rising period of the drive frequency by the lighting control of this invention. It is an example of the wave form diagram in the starting period of the drive current by lighting control of this invention, a starting period, and a steady period.

Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.
In addition, in the drawings used in the following description, in order to make the features easy to understand, there are cases where the portions that become the features are enlarged for the sake of convenience, and the dimensional ratios of the respective components are not always the same as the actual ones. Absent.

(projector)
FIG. 1 is a block diagram illustrating a configuration example of the projector 1 according to the present embodiment.
As shown in FIG. 1, the projector 1 includes a discharge lamp (light source) 10 that irradiates illumination light L, and a liquid crystal panel (light modulation device) that forms image light L ′ obtained by modulating the illumination light L according to image data. ) 20 and a projection optical system 30 that projects the image light L ′ onto a screen (not shown).

  In this embodiment, the case where an ultra-high pressure mercury lamp using arc discharge is used as the discharge lamp 10 is exemplified, but the present invention is not limited to this, and an arbitrary discharge lamp such as a metal halide lamp or a xenon lamp is used. Can be used.

  Further, the projector 1 schematically includes an interface (I / F) unit 40, an image processing unit 50, a liquid crystal panel driving unit 60, a discharge lamp lighting device 70, and a CPU (Central Processing Unit) 80.

  The interface unit 40 converts an image signal input from a personal computer (not shown) into image data in a format that can be processed by the image processing unit 50.

  The image processing unit 50 performs various image processing such as luminance adjustment and color balance adjustment on the image data supplied from the interface unit 40.

  The liquid crystal panel driving unit 60 is for driving the liquid crystal panel 20 based on the image data subjected to the image processing by the image processing unit 50.

  The discharge lamp lighting device 70 controls the lighting of the discharge lamp 10, and a high-frequency voltage of about several tens of kHz between a pair of electrodes of the discharge lamp 10 using a resonance circuit unit 73 described later when starting the discharge lamp 10. Is applied. After starting, an operation of lowering the driving frequency of the discharge lamp 10 to a steady frequency (about several hundred Hz) lower than the resonance frequency is performed, and steady lighting is performed at the steady frequency.

  The CPU 80 controls the image processing unit 50 and the projection optical system 30 in accordance with an operation of a remote controller (not shown) or an operation button provided on the main body of the projector 1 or the like.

  In the present embodiment, for example, when the user operates a power switch (not shown) of the projector 1, the CPU 80 outputs a control signal for lighting the discharge lamp 10 to the discharge lamp lighting device 70. .

(Discharge lamp lighting device)
FIG. 2 is a block diagram illustrating a configuration example of the discharge lamp lighting device 70 according to the present embodiment.
As shown in FIG. 2, the discharge lamp lighting device 70 includes a down chopper unit 71, a power conversion unit 72, a resonance circuit unit 73, a voltage detection unit 74, a lighting detection unit 75, and a control unit 76. Outline Among these, the down chopper unit 71, the power conversion unit 72, and the resonance circuit unit 73 constitute a drive unit 77 that drives the discharge lamp 10.

  The down chopper unit 71 converts DC power having a voltage Vin applied from a DC power source (not shown) between the input terminal TIN1 and the input terminal TIN2 into DC power having a predetermined DC voltage. Type field effect transistor (FET) 711, choke coil 712, diode 713, and capacitor 714.

  In the down chopper unit 71, the DC power having a desired output voltage corresponding to the duty ratio of the control signal S711 is obtained by chopping the current flowing through the FET 711 based on the control signal S711 supplied from the control unit 76. Can be obtained. Note that the down chopper 71 is not an essential component for the discharge lamp lighting device 70 according to the present embodiment, and may be omitted as necessary.

  The power conversion unit 72 converts the DC power supplied from the down chopper unit 71 into AC power, and supplies the AC power to the discharge lamp 10 via the resonance circuit unit 73. It is constituted by a full bridge circuit composed of n-channel field effect transistors (FETs) 721 to 724.

  That is, among the FETs 721 to 724 constituting the full bridge circuit, the drains of the FETs 721 and 722 are connected to the high potential node NH connected to the input terminal TIN1 via the FET 711 and the choke coil 712 constituting the down chopper unit 71. ing. The sources of the FETs 721 and 722 are connected to the drains of the FETs 723 and 724, respectively. The sources of the FETs 723 and 724 are connected to a low potential node NL connected to the input terminal TIN2 via a resistor 751 constituting a lighting detection unit 75 described later.

  A control signal Sa is supplied from the control unit 76 to the gates of the FETs 721 and 724, and a control signal Sb corresponding to an inverted signal of the control signal Sa is supplied from the control unit 76 to the gates of the FET transistors 722 and 723. .

  In the present embodiment, the connection between the source of the FET 721 and the drain of the FET 723 is one output node N1 of the power converter 72, and the connection between the source of the FET 722 and the drain of the FET 724 is the power converter 72. The other output node N2 is used.

  In the power conversion unit 72, the pair of FETs 722 and 723 and the pair of FETs 721 and 724 perform a complementary switching operation based on the control signal S (Sa, Sb) supplied from the control unit 76. It is possible to convert electric power into AC power.

  In the present embodiment, the power conversion unit 72 is configured by a full bridge circuit. However, as long as AC power can be supplied to the resonance circuit unit 73, the circuit format of the power conversion unit 72 is a half bridge circuit or the like. Any circuit format may be used.

  The resonance circuit unit 73 functions as an igniter that generates a high voltage exceeding the discharge start voltage (breakdown voltage) of the discharge lamp 10, and is in parallel with the power conversion unit 72 via the output terminals TOUT1 and TOUT2. Connected to the discharge lamp 10.

  The resonance circuit unit 73 includes two coils 731 and 732 that are magnetically coupled and a capacitor 733. Among these, one end of the coil 731 is connected to the output node N1 of the power converter 72, the other end of the coil 731 is connected to one end of the coil 732, and the other end of the coil 732 is connected to the output terminal TOUT1. . In addition, one electrode of a capacitor 733 is connected to a connection node between the coil 731 and the coil 732, and the other electrode of the capacitor 733 is connected to the output node N <b> 2 of the power conversion unit 72 and output. It is connected to the terminal TOUT2.

  In this embodiment, an LC series resonance circuit is formed by the coil 731 and the capacitor 733 constituting the resonance circuit unit 73. Basically, the resonance frequency of the LC series resonance circuit (resonance determined by the coil 731 and the capacitor 733). Frequency) is a resonance frequency specific to the resonance circuit unit 73. Therefore, in principle, if the frequency of the AC power supplied from the power conversion unit 72 matches the resonance frequency of the resonance circuit unit 73 and the LC series resonance circuit composed of the coil 731 and the capacitor 733 enters a resonance state, The voltage V733 between the terminals of the capacitor 733 becomes infinite, and a high voltage necessary for starting the discharge of the discharge lamp 10 is obtained by the resonance circuit unit 73.

  Here, even if the LC series resonance circuit is in a resonance state, if there are resistance components and wiring impedances of the FET transistors 721 to 724 constituting the power conversion unit 72, the voltage V733 between terminals of the capacitor 733 is approximately 1-1. The high voltage required to start the discharge of the discharge lamp 10 cannot be obtained.

  Therefore, in the present embodiment, a coil 732 that is magnetically coupled to the coil 731 constituting the LC series resonance circuit is disposed, and the voltage V733 between the terminals of the capacitor 733 is set according to the turns ratio of the coil 731 and the coil 732. As a result, the high voltage (resonance voltage) of several kV necessary to finally start the discharge of the discharge lamp 10 is generated.

  The resonance voltage detection unit 74 is for detecting a voltage V733 between terminals of the capacitor 733 constituting the resonance circuit unit 73. The resistor 741 and the resistor 742 connected in series between the terminals of the capacitor 733, and an analog / Digital (A / D) conversion unit 743.

  Among these, the resistor 741 and the resistor 742 are for dividing the voltage V733 between the terminals of the capacitor 733 of the resonance circuit unit 73 to obtain a voltage V74 according to the resistance ratio.

  On the other hand, the analog / digital conversion unit 743 converts the divided voltage V74 into digital data and outputs the digital data. In the present embodiment, the divided voltage V74 is an intermediate voltage generated in order to adapt the voltage V733 to the input characteristics of the analog / digital converter 743. Therefore, the digital data output from the analog / digital conversion unit 743 represents the value of the voltage V733, and the voltage V733 detected by the voltage detection unit 74 is supplied to the control unit 76.

  The lighting detection unit 75 detects lighting / non-lighting of the discharge lamp 10, and includes a resistor 751 and a comparator unit 752.

  Among these, the resistor 751 is connected between the input terminal TIN <b> 2 and the sources of the FETs 723 and 724 constituting the power conversion unit 72, and the voltage between the terminals (drop voltage) of the resistor 751 is input to the comparator unit 752. Is done.

  The comparator 752 detects the current flowing through the discharge lamp 10 based on the voltage between the terminals of the resistor 751, and the detected current and a predetermined current corresponding to the current flowing through the resistor 751 when the discharge lamp 10 is turned on. The lighting / non-lighting of the discharge lamp 10 is detected by comparing with a voltage value (not shown).

  That is, for example, when the voltage between the terminals of the resistor 751 is equal to or higher than a predetermined voltage value, the lighting detection unit 75 detects the lighting of the discharge lamp 10. On the other hand, when the voltage between the terminals of the resistor 751 falls below a predetermined voltage value, the non-lighting of the discharge lamp 10 is detected. When the lighting detection unit 75 detects the lighting of the discharge lamp, the lighting detection unit 75 outputs a signal indicating that to the control unit 76.

  The control unit 76 controls each switching operation of the down chopper unit 71 and the power conversion unit 72 described above. The control unit 76 includes a voltage control oscillator 761. The voltage controlled oscillator 761 outputs a signal having a frequency corresponding to an input voltage (not shown) as a control signal S. The signal defining the input voltage of the voltage controlled oscillator 761 is generated in the control unit 76 so that the switching operation of the power conversion unit 72 can be obtained.

(Discharge lamp lighting method)
FIG. 3 is a diagram for explaining the lighting control (discharge lamp lighting method) of the discharge lamp lighting device 70 according to the present embodiment. FIG. 3A is supplied to the discharge lamp 10 in the conventional lighting control. FIG. 3B shows an example of a waveform diagram of the drive current supplied to the discharge lamp 10 in the lighting control of the present invention.

  Here, in the present embodiment, a period A during which the discharge lamp 10 is driven at the resonance frequency when the discharge lamp 10 is started is referred to as a “starting period”, and after this starting period A, the driving frequency of the discharge lamp 10 is determined from the resonance frequency. A period B until the lower steady frequency is lowered is referred to as a “rising period”, and a period C during which the discharge lamp 10 is driven at a steady frequency after the rising period B is a “steady period” (not shown in FIG. 3). And

  In the conventional lighting control, as shown in FIG. 3A, when a resonant voltage is applied between a pair of electrodes of the discharge lamp 10 by starting the discharge lamp 10, the discharge lamp 10 causes dielectric breakdown. The discharge of the discharge lamp 10 is started. The discharge lamp 10 generates glow discharge after starting lighting, and then shifts from glow discharge to arc discharge. At this time, a state occurs (one half-wave discharge) in which the electrode on one side of the discharge lamp 10 does not shift from glow discharge to arc discharge. In the present embodiment, a period D from the transition from the glow discharge to the arc discharge until the start period A ends is referred to as an “arc start period”.

  Immediately after the end of the starting period A, the power (current, voltage) supplied to the discharge lamp 10 gradually increases, and it takes some time until a stable steady lighting state is achieved. Therefore, the start-up period B after the end of the start period A is a period for stabilizing the lighting state of the discharge lamp 10.

  The waveform diagram of the drive current shown in FIG. 3A represents a state in which the half wave discharge generated in the discharge lamp 10 does not shift to full wave discharge in the arc starting period D. In this case, a spatter phenomenon due to glow discharge occurs and blackening occurs. Further, when the half-wave discharge is shifted to steady lighting, the discharge becomes unstable, and the discharge lamp 10 is extinguished in some cases.

  On the other hand, in the lighting control according to the present invention, as shown in FIG. 3B, at least the discharge lamp 10 is supplied in the arc starting period D after the discharge lamp 10 shifts from glow discharge to arc discharge. An amplification period E for amplifying the drive current is provided.

  Specifically, in the lighting control of the present invention, in order to promote the transition from glow discharge to arc discharge, in the amplification period E, the drive current supplied to the discharge lamp 10 is amplified to activate the release of thermoelectrons at the electrodes. Make it. Thereby, the half-wave discharge generated in the discharge lamp 10 can be appropriately and easily transferred to the full-wave discharge.

Further, the amplification period E, it is desirable to provide an intermediate t _M of the arc starting period D during the period leading to the termination. That is, in the present embodiment, the current value of the drive current supplied to the discharge lamp 10 is amplified only during t ₁ to t ₂ within this period.

  As described above, in the lighting control according to the present invention, the function of detecting the half-wave discharge is not added to the control unit 76, and is temporarily applied between the pair of electrodes of the discharge lamp 10 when the discharge lamp 10 is started. Control is performed to increase the resonance voltage.

Accordingly, the electrode that is not shifted to the arc discharge is warmed up to an intermediate t _M of the arc starting period from D, the thermionic emission progresses to some extent, the process proceeds to arc discharge and the subsequent current amplification in the wake It becomes easy. Therefore, by limiting the current amplification time and preventing the drive current from flowing excessively to the discharge lamp 10, the shape of the electrode protrusion can be suppressed while suppressing the above-described damage caused by blackening or tube wall discharge. It is possible to maintain.

  The waveform diagram of the drive current shown in FIG. 3B shows a half of the current generated in the discharge lamp 10 by providing an amplification period E for amplifying the drive current supplied to the discharge lamp 10 in the arc starting period D. It represents the situation where wave discharge has shifted to full wave discharge.

  According to the lighting control of the present invention, it is possible to appropriately and easily shift the half wave discharge generated in the discharge lamp 10 to the full wave discharge while reducing the load applied to the discharge lamp 10.

  In the amplification period E, it is desirable that the effective value of the drive current supplied to the discharge lamp 10 is amplified by about 20 to 30% with respect to the reference current value at the start of the discharge lamp 10. For example, in the present embodiment, the current value in the amplification period E is amplified to 2.5 A with respect to the reference current value 2.0 A.

  Further, the method for amplifying the drive current supplied to the discharge lamp 10 is not particularly limited. For example, the method for changing the drive frequency of the discharge lamp 10 or the method for changing the output voltage of the down chopper 71 is used. Etc. can be used.

FIG. 4 is an example of a waveform diagram in the drive current rising period B by the lighting control of the present invention.
In the lighting control according to the present invention, in addition to the control of the driving current in the starting period A described above, the driving supplied to the discharge lamp 10 simultaneously with the start of the rising period B in the rising period B shown in FIG. While reducing the current, control is performed to amplify the drive current supplied to the discharge lamp 10 stepwise or continuously until the end of the start-up period B. 4A shows an example of a waveform diagram when the drive current is amplified stepwise, and FIG. 4B shows an example of a waveform diagram when the drive current is amplified continuously. Represent.

  In this case, the driving current supplied to the discharge lamp 10 is reduced simultaneously with the start of the start-up period B, so that a half-wave discharge is not eliminated in the discharge lamp 10 and a tube wall discharge occurs. Even if it is, the load applied to the discharge lamp 10 can be reduced. In addition, after the drive current is reduced, the drive current supplied to the discharge lamp 10 is amplified stepwise or continuously until the end of the start-up period B, thereby reducing the temperature in the discharge lamp 10. It is possible to suppress the occurrence of blackening due to.

FIG. 5 is an example of a waveform diagram in the driving frequency rising period B by the lighting control of the present invention.
In the lighting control of the present invention, in addition to the control of the driving current in the rising period B described above, in the rising period B shown in FIG. 5, this rising period B is divided into a plurality of periods B ₁ , B ₂ , B _3. And at the same time B ₁ , B ₂ , B ₃ , control is performed to lower the driving frequency of the discharge lamp 10.

In other words, in the lighting control of the present invention, the rising period B a plurality of periods obtained by dividing _{B 1,} of the B 2, _{B 3,} the period and the driving frequency _{f 1} in _{B 1,} the driving frequency _{f 2} in the period _{B 2} When performed sequentially lowering controls the drive frequency _{f 3} in the period _{B 3 (f 1> f 2} > f 3).

In this case, a sudden change when the starting period high in A (about several tens kHz) the resonance frequency f _A low in the steady period C (about several hundreds Hz) until a steady frequency f _C lowering the driving frequency of the discharge lamp 10 Can be suppressed.

  That is, there is a large difference in the driving frequency of the discharge lamp 10 between the start period A and the steady period C described above. For this reason, if the driving frequency of the discharge lamp 10 is suddenly changed, the electrode of the discharge lamp 10 is deformed or the discharge of the discharge lamp 10 becomes unstable. In this case, the illuminance reduction or flickering of the discharge lamp 10 may be caused.

On the other hand, in the lighting control of the present invention, the drive frequency in the start-up period B is set lower than the start period A and higher than the steady period C. Further, the start-up period B is divided into a plurality of periods B ₁ , B ₂ , B _3, and control is performed to gradually lower the drive frequency for each of the divided periods B ₁ , B ₂ , B ₃ .

  As a result, a rapid change in the driving frequency from the starting period A to the steady period C can be suppressed, and the discharge lamp 10 can be stably brought into a steady lighting state while maintaining the protruding shape of the electrodes in the discharge lamp 10. It is possible to migrate.

Further, immediately after the transition to the start-up period B, the temperature of the discharge lamp 10 is lower than when the transition to the steady period C, so that the tungsten forming the electrodes is likely to solidify and blackening is likely to occur. On the other hand, in the period B ₁ immediately after the transition to the start-up period B, the discharge lamp 10 is driven at a higher frequency than the subsequent periods B ₂ and B ₃ , so that the polarity of the electrodes in the discharge lamp 10 is On the other hand, the bias time is shortened, and the transpiration of tungsten is suppressed. Therefore, there is a merit that the risk of occurrence of blackening described above can be suppressed.

Specifically, in the period B ₁ , the driving frequency f ₁ of the discharge lamp 10 is preferably in the range of several kHz, more specifically in the range of 0.5 kHz to 10 kHz, and more preferably 1 ± 0. The range is 2 kHz. As a result, the time during which the polarity of the electrode in the discharge lamp 10 is biased to one side is shortened and the transpiration of tungsten is suppressed, so that the occurrence of blackening described above can be suppressed.

In the present embodiment, the case where the rising period B is divided into _three periods B ₁ , B ₂ , and B ₃ is illustrated. However, the present invention is not limited to this case, and the rising period B is at least 2 Control may be performed in which the driving frequency is divided into two or more periods and the driving frequency is lowered for each of the divided periods. In the present embodiment, there is no particular need to define the upper limit of the number of divisions when the rising period B is divided into a plurality of periods. In some cases, the driving frequency is continuously set in the rising period B. It is also possible to perform control to lower the value.

FIG. 6 is an example of a waveform diagram in the starting period A, the rising period B, and the steady period C of the drive current by the lighting control of the present invention.
The waveform diagram of the drive current shown in FIG. 6 includes the control of the drive current in the start period A shown in FIG. 3B and the control of the drive current in the rising period B shown in FIG. This is a combination of the control of the driving frequency in the rising period B shown in FIG.

Of these, the rising period B, the start-up period B is divided into a plurality of periods _{B 1,} B 2, _{B 3,} among the divided period _{B 1,} B 2, _{B 3,} rising period B In the period B ₁ immediately after the transition to, the drive current supplied to the discharge lamp 10 is reduced, and the drive current supplied to the discharge lamp 10 is gradually (or continuously) until the end of the period B _1. The control of amplification may be performed.

  As described above, by performing the lighting control of the discharge lamp 10 according to the present invention, a half wave generated in the discharge lamp 10 during the period from the start of the discharge lamp 10 to the steady lighting of the discharge lamp 10. It is possible to appropriately and easily shift the discharge to the full wave discharge. Further, in the process from starting the discharge lamp 10 to steady lighting, it is possible to reduce the risk of blackening, tube wall discharge, and the discharge lamp 10 going off.

  Therefore, the projector 1 includes the discharge lamp lighting device 70 that performs the lighting control according to the present invention, so that the lighting control of the discharge lamp 10 with excellent reliability can be performed. It is possible to extend the life and improve the quality.

  DESCRIPTION OF SYMBOLS 1 ... Projector 10 ... Discharge lamp (light source) 20 ... Liquid crystal panel (light modulation device) 30 ... Projection optical system 40 ... Interface part 50 ... Image processing part 60 ... Liquid crystal panel drive part 70 ... Discharge lamp lighting device 71 ... Down chopper part 72 ... Power conversion unit 73 ... Resonance circuit unit 74 ... Voltage detection unit 75 ... Lighting detection unit 76 ... Control unit 77 ... Drive unit 80 ... CPU A ... Start-up period B ... Startup period C ... Steady period D ... Arc start-up period E … Amplification period

Claims (8)

A drive unit for driving the discharge lamp by supplying a drive current to the discharge lamp;
A control unit for controlling the drive unit,
The drive unit has a resonance circuit unit that generates a high voltage for starting discharge of the discharge lamp,
The control unit includes a start period that is a first frequency for generating the high voltage, a start-up period until the discharge lamp transitions to steady lighting after the start period, and the steady lighting after the start-up period. It said drive unit is controlled so that the driving current including a constant period to be a second frequency lower than the first frequency, a is supplied to the discharge lamp,
The control unit provides an amplification period for amplifying a drive current supplied to the discharge lamp after a predetermined period in the start period,
Wherein the control unit, a discharge lamp lighting apparatus characterized by reducing the drive current supplied to Oite the discharge lamp from the start-up period to the transition to the startup period. The discharge lamp lighting device according to claim 1,
The start period includes an arc start period from when the discharge lamp has shifted from glow discharge to arc discharge until the start period ends,
The discharge lamp lighting device, wherein the amplification period is provided in the arc start period. The discharge lamp lighting device according to claim 2,
The discharge lamp lighting device, wherein the amplification period is provided in the second half of the arc starting period. The discharge lamp lighting device according to any one of claims 1 to 3,
The controller is configured to amplify a drive current supplied to the discharge lamp stepwise or continuously in the start-up period. The discharge lamp lighting device according to any one of claims 1 to 4,
The controller supplies a driving current having a third frequency lower than the first frequency and higher than the second frequency to the discharge lamp during the start-up period. The discharge lamp lighting device according to any one of claims 1 to 5,
The discharge lamp lighting device, wherein the control unit gradually decreases the frequency of the drive current supplied to the discharge lamp during the start-up period. A discharge lamp lighting method for controlling the lighting of the discharge lamp by supplying a driving current to the discharge lamp,
In a starting period of a first frequency for generating a high voltage for starting discharge of the discharge lamp, a rising period until the discharge lamp shifts to steady lighting after the starting period, and in the steady lighting after the rising period a drive current and a constant period to be the second frequency lower than the first frequency is supplied to the discharge lamp,
In the start-up period, an amplification period for amplifying a drive current supplied to the discharge lamp after a predetermined period is provided,
Discharge lamp lighting method characterized by reducing the drive current supplied to Oite the discharge lamp the transition to the startup period from the start-up period. The discharge lamp emitting light;
The discharge lamp lighting device according to any one of claims 1 to 6,
A light modulation device that modulates light from the discharge lamp according to image data;
And a projection optical system that projects the light modulated by the light modulation device.

Images