Discharge lamp lighting circuit

A discharge lamp lighting circuit includes an emission acceleration controller for detecting a lamp voltage for the discharge lamp, and supplying power greater than a rated value when the discharge lamp is initially lighted, and for gradually reducing the power supplied thereafter so as to shift the discharge lamp to a steady state. Power control is provided so that the power supplied to the discharge lamp is reduced in accordance with a rise in the voltage of a capacitor, and a charge current is supplied to the capacitor by current sources that provide a current that depends on the time elapsed since the lighting of the discharge lamp started and a second current that depends on a lamp voltage.

This application claims foreign priority based on Japanese patent application JP 2003-190253, filed on Jul. 2, 2003, the contents of which is incorporated herein by reference in its entirety.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a discharge lamp lighting circuit which uses a capacitor to control the supply of transient power to obtain a satisfactory starting performance for a discharge lamp.

2. Description of the Related Art

A related art discharge lamp lighting circuit configuration includes a direct-current power source circuit, a DC-AC converter and a starting circuit (i.e., a starter). With this related art configuration, the discharge lamp lighting circuit (while in a steady state) supplies a rated power to a discharge lamp.

To quickly raise the luminous flux of the discharge lamp, during a transition period immediately following the lighting of the discharge lamp, power exceeding the rated power is supplied to the discharge lamp to accelerate the emission of light (see JP-A-9-330795, for example).

For a related art circuit for lighting a discharge lamp containing mercury, for example, during a transition period extending from immediately following the lighting of the discharge lamp until it is shifted to the steady state, a lamp current (or power to be supplied) corresponding to a lamp voltage is regulated, i.e., a control process is performed based on a so-called control line.

For a lighting circuit for a discharge lamp that contains either no mercury or only a small amount of mercury, starting performance variances constitute a problem when the control method employed uses a control line as a reference. Therefore, predictive control is required for the change in power.

However, with the related art configuration, there are various inconveniences associated with the control arrangement for reducing the starting time for a discharge lamp.

For example but not by way of limitation, costs rise because either the structure of a circuit is complicated or the scale of the circuit is increased. Further, there is a design problem (e.g., that there is nothing in common with the circuit structure for a discharge lamp that contains mercury and the circuit structure for a discharge lamp that contains no mercury or only a small amount of mercury) and the multiplicity of the use of the circuit is poor.

SUMMARY OF THE INVENTION

It is an object of the present invention to provide a discharge lamp lighting circuit which can increase the starting performance of a discharge lamp without complicating the circuit structure or increasing the circuit size. However, the present invention can be realized without this object, or any object.

To achieve this objective, the invention includes the following configuration.

A discharge lamp lighting circuit includes an emission acceleration controller for detecting a lamp voltage for a discharge lamp and for supplying power greater than a rated value when the discharge lamp is initially lighted, and for, thereafter, gradually reducing the supplied power to shift the discharge lamp to a steady state.

Power control is provided so that the power supplied to the discharge lamp is reduced in accordance with a rise in the voltage of a capacitor that constitutes the emission acceleration controller.

A charge current is supplied to the capacitor, which constitutes the capacitor of the emission acceleration controller, by a plurality of current sources that provide a first current, which depends on the time that has elapsed since the lighting of the discharge lamp started, and a second current, which depends on a lamp voltage.

Therefore, according to this invention, to control power supplied to the discharge lamp during a transition period, a capacitor is provided that constitutes an emission acceleration controller and that is charged by using currents supplied by a plurality of power sources. With this arrangement, the circuit structure can be simplified without a control line. The configuration of this invention can be applied regardless of whether a discharge lamp contains mercury, as a luminous material, or contains no mercury or only a small amount. For example, when the invention is employed for a lighting circuit for a discharge lamp that does not contain mercury, the starting period can be reduced and stabilized Thus, the occurrence of overshoot or undershoot can be prevented in accordance with the rising characteristic of a luminous flux.

DETAILED DESCRIPTION OF THE INVENTION

An exemplary, non-limiting embodiment of the present invention is shown inFIG. 1. A discharge lamp lighting circuit1comprises a direct-current power source2, a DC—DC converter3, a DC-AC converter4and a starting circuit5.

The DC—DC converter3raises or lowers the voltage of a current received from the DC power source2, and outputs a desired DC voltage. The output voltage of the DC—DC converter3varies in accordance with a control signal received from a controller7, as described below. The DC—DC converter3can be a DC—DC converter (e.g., a chopper or a flyback type) having a switching regulator.

The DC-AC converter4changes the output voltage of the DC—DC converter3into an AC voltage, and supplies the AC voltage to a discharge lamp6. The DC-AC converter4can include a bridge circuit (a full bridge circuit or a half bridge circuit) including a plurality of semiconductor switching devices, and a driver for the bridge circuit.

The starting circuit5generates a high voltage signal (start pulse) and supplies this signal to the discharge lamp6to be activated. The high voltage signal is superimposed with the AC voltage output by the DC-AC converter4, and the resultant signal is applied to the discharge lamp6. In this exemplary, non-limiting embodiment, the discharge lamp6either contains mercury, does not contain mercury or contains only a small amount of mercury.

The following arrangements can be employed for a detector for detecting the voltage or the current of the discharge lamp6.

(A) To directly detect the voltage or the current of a discharge lamp, a current detection device (a shunt resistor or a detection transformer) is connected to the discharge lamp to detect the current across the current detection device.

(B) An equivalent voltage for the lamp voltage, or the lamp current of a discharge lamp, is detected.

InFIG. 1, the arrangement (B) is shown, and a detector8is between the DC—DC converter3and the DC-AC converter4. The detector8includes a voltage divided resistor8a, a voltage detector for detecting a DC output voltage using the voltage-divided resistor8a, and a current detector using a current detection resistor8b. The detection signals are transmitted to the controller7.

The controller7has a power control function in the steady state of the discharge lamp6and a power control function in the transient state. The controller7controls the power supplied to the discharge lamp6in the steady state (constant power control), in accordance with a detection signal for the voltage applied to the discharge lamp6, and a detection signal for the current flowing through the discharge lamp6.

Also, before performing this power control process, the controller7controls the output of the DC—DC converter3to control the power supplied to the discharge lamp6during a transition period. The controller7includes a function for driving the DC-AC converter4and a fail-safe function for determining when an abnormality has occurred in the state or the operation of the circuit.

In the controller7, an emission acceleration controller9relates to the present invention detects a lamp voltage for the discharge lamp6, supplies power having a rated value when the discharge lamp6is initially lighted, and gradually reduces the supplied power thereafter to shift the discharge lamp6to the steady state. The emission acceleration controller9also provides power control, so that the power supplied to the discharge lamp6is reduced in accordance with a rise in the voltage of a capacitor10that constitutes the emission acceleration controller9(inFIG. 1, the capacitor10is an external device).

For a discharge lamp that contains mercury, since the lamp voltage rises prior to the rise in the luminous flux, the power that is to be supplied can be controlled while the lamp voltage is monitored. For a discharge lamp that contains no mercury, or only a small amount, the lamp voltage rise does not always occur prior to the rise in the luminous flux. Thus, predictive control is required for a change in the power supplied during the transition period.

FIG. 2is a schematic diagram for explaining the emission acceleration controller9, and illustrates the capacitor10, a plurality of current sources11and12, a power controller13, an operation controller14and an essential portion of the DC—DC converter3.

The current source11(the current value is referred to as an “I1”) and the current source12(the current value is referred to as an “I2”) are provided for the capacitor10. These current sources are variable current sources. The charge current I1supplied by the current source11to the capacitor10depends on the time that has elapsed since the start of the lighting of the discharge lamp6. The charge current I2, supplied by the current source12to the capacitor10, is changed, depending on the level of the lamp voltage. That is, the current I1or I2, or a current “I1+I2”, is supplied by the current source to the capacitor10in accordance with the state of the discharge lamp6.

The power controller13includes an error amplifier13afor power calculation, and a power control and addition unit13b. The terminal voltage of the capacitor10(hereinafter referred to as “VC”) is applied to the error amplifier13athrough the power control and addition unit13b. As a result, more power is added to the constant power, and the obtained power is supplied to the error amplifier13a. When the voltage VC of the capacitor10is increased by the charge current supplied by the current source11or12, transient power control is provided to reduce the power supplied to the discharge lamp6in accordance with the rise in the voltage. At the succeeding stage, the power controller13transmits to the operation controller14a control output consonant with the VC.

The operation controller14receives a control signal from the power controller13and controls the output of the DC—DC converter3. Based on the results obtained by comparing the level of the control voltage applied by the power controller13with the level of a lamp wave supplied by a circuit (not shown), a control signal is transmitted to the DC—DC converter3, and a switching device, such as an FET that constitutes the DC—DC converter3, is driven.

InFIG. 2, a flyback configuration including a transformer T and a switching device SW is shown, and a rectifying and smoothing circuit15, constituted by a diode D and a capacitor C, is provided on the secondary side of the transformer T. When the PWM (Pulse Width Modulation) method is employed as a switching method, a PWM comparator constituting the operation controller14obtains a signal pulse having a rectangular wave shape (PWM pulse) by performing a level comparison with the lamp wave, and transmits the pulse signal through a buffer (not shown) to the control terminal (the gate of the FET) of the switching device SW. The PFM (Pulse Frequency Modulation) may be employed as another switching method.

FIG. 3is a schematic graph showing the time-transient change in power, while the horizontal axis represents a time “t” that has elapsed since the lighting start, and the vertical axis represents a power “P”, which is supplied to the discharge lamp6.

Graph segments ga, gb and gc inFIG. 3are defined as follows.

“ga”: a line segment representing the maximum value “Pmax” of the power supplied to the discharge lamp6

“gb”: a line segment related to the emission acceleration control for the discharge lamp6, and inclined right upward to connect the segments ga and gc

“gc”: a line segment representing the rated value “Pc” of the power supplied to the discharge lamp6

When the VC of the capacitor10is zero, as is indicated by the graph line ga, the power Pmax is output for supply to the discharge lamp6. As the voltage VC is increased, the power P is reduced. When the voltage VC reaches a predetermined voltage (hereinafter referred to as an “Eref”), the rated power Pc is output.

FIG. 4is a diagram showing an exemplary, non-limiting circuit configuration16for emission accelerating control. A constant voltage source17for supplying the voltage Eref is connected to the capacitor10through three series resistors18,19and20to constitute the current source11.

A circuit unit23, including an NPN transistor21and a resistor22, is provided in parallel to the resistor18. The collector for the NPN transistor21is connected to the constant voltage source17and the emitter of the NPN transistor21is connected to respective nodes of the resistors18and19. A predetermined voltage (hereinafter referred to as a “Vcc”) is applied to the base of the NPN transistor21through the resistor22.

A circuit unit28, including an NPN transistor24, resistors25and26and a comparator27, is provided for the resistor19. The collector of the NPN transistor24is connected to the node of the resistors18and19, and the emitter of the NPN transistor24is connected to a node of the resistors19and20. The base of the NPN transistor21is connected to the output terminal of the comparator27through the resistor25.

The negative input terminal of the comparator27is connected to the capacitor10. The positive input terminal of the comparator27is connected to the positive input terminal of a comparator45described below. The voltage Eref is applied to the resistor26connected to the output terminal of the comparator27.

A lamp voltage detector29, a current mirror circuit30and circuit units31and32are provided as a system for supplying the current I2to the capacitor10.

The lamp voltage detector29applies a detected voltage (hereinafter referred to as a “Vs”), which corresponds to the lamp voltage VL of the discharge lamp6, through an amplifier33to the non-inversion input terminal of an operating amplifier34. The signal output by the operating amplifier34is transmitted to the base of an NPN transistor35. The emitter of the NPN transistor35is connected to the inversion input terminal of the operating amplifier34and is grounded through a resistor36.

The current mirror circuit30is constituted by using a plurality of PNP transistors37to39.

The collector of the PNP transistor37is connected to the collector of the NPN transistor35, and the predetermined voltage Vcc is applied to the emitter of the PNP transistor37through a resistor40.

The collector of the PNP transistor38is grounded, the base of the PNP transistor38is connected to the collector of the PNP transistor37, and the emitter of the PNP transistor38is connected to the base of the PNP transistor37.

The base of the PNP transistor39is connected to the base of the PNP transistor37and the emitter of the PNP transistor38. The predetermined voltage Vcc is applied to the emitter of the PNP transistor39through a resistor41.

The collector of the PNP transistor39is connected to the anode of a diode42, and the cathode of the diode42is connected to the capacitor10to supply the current I2to the capacitor10.

The circuit unit31is constituted by three comparators43,44and45. The detected voltage Vs indicating the lamp voltage VL is applied to the positive input terminal of the comparator43, and a predetermined reference voltage (hereinafter referred to as an “E2”) is applied to the negative input terminal of the comparator43. The output terminal of the comparator43is connected to the collector of the PNP transistor39.

The positive input terminal of the comparator44is connected to the capacitor10(or the cathode of the diode42), and a predetermined reference voltage (hereinafter referred to as an “E1”) is applied to the negative input terminal of the comparator44. The output terminal of the comparator44is connected to the collector of the PNP transistor39.

The negative input terminal of the comparator45is connected to the capacitor10, and a predetermined reference voltage (hereinafter referred to as an “E4”) is applied to the positive input terminal of the comparator45. The output terminal of the comparator45is connected to the collector of the PNP transistor39, and the reference voltage E4is also applied to the positive input terminal of the comparator45.

The circuit unit32is constituted by using a comparator46and a resistor47. The negative terminal of the comparator46is connected to the capacitor10, a predetermined reference voltage (hereinafter referred to as an “E3”) is applied to the positive input terminal of the comparator46, and the output terminal of the comparator46is connected to the collector of the PNP transistor39through the resistor47.

The operation of the thus arranged lighting circuit will now be described while referring toFIG. 5.

FIG. 5is a graph showing exemplary, non-limiting segments of a control area. The horizontal axis represents time “t” and the vertical axis represents the voltage VC of the capacitor10to show the time-transient change in the voltage VC. The voltages E1to E4and Eref are defined as described above, and the relationship of the voltage levels E1<E3<E4<Eref is established.

For the emission acceleration control for shifting, from the start of the lighting, the discharge lamp6to the steady state, the control area is divided into a plurality of control area segments (A to C). The control area is divided into multiple segments, so that for each area segment, the change in the power supplied to the discharge lamp6(reduction rate) can be controlled. For example, the supply of the current I1or I2to the capacitor10is permitted for a specific control area segment, and is inhibited for another control area segment, so that the rate at which the voltage of the capacitor10is increased (i.e., the rate at which the power supplied to the discharge lamp6is reduced) can be controlled.

The control area segments A to C are provided. As is shown inFIG. 5, the degree to which the voltage VC is increased differs depending on the area segments.

The first area A corresponds to a period during which the supply of a power larger than a rated value is required, while taking into account the time required for the iodide contained in the discharge lamp to evaporate. Since in the second area B the luminous flux rises sharply in accordance with the evaporation of the iodide, the power supplied to the discharge lamp6must be quickly reduced. Therefore, in the second area B, the rate at which the voltage VC is increased is greater than in the other areas. In the third area C, the lamp voltage VL is indicated as an almost steady value; however, since the temperature of the discharge lamp6has not yet reached the temperature of the steady state, the power supplied to the discharge lamp6must be gradually reduced near the rated value (the range following the point whereat VC=Eref is established corresponds to the steady area).

It is preferable that the level of the terminal voltage of the capacitor10or the level of the lamp voltage VL be employed to determine the shifting of the emission acceleration control from a specific control area segment to another control area segment. However, the present invention is not limited thereto, and other equivalents as would be understood by one of ordinary skill in the art may be substituted therefore.

For the operation of the lighting circuit in the first area A, the NPN transistor21of the circuit unit23is turned on, and since VC<E4is established, the NPN transistor24is turned on in accordance with an H (high) signal that is output by the comparator27of the circuit unit28. Therefore, the current I1, from the constant voltage source17, is supplied through the resistor20to the capacitor10.

The supply of the current I2to the capacitor10is halted in accordance with L (low) signals that are output by the comparators43and44of the circuit unit31.

Therefore, the rate at which power supplied to the discharge lamp6is reduced is defined as the rate at which the voltage VC is increased when the capacitor10is charged by receiving, through the resistor20, the current I1consonant with a specific time constant. That is, in the first area A at the initial time during the period of the transition to the steady state, only the current I1is supplied to the capacitor10, and the degree of the rise in the voltage of the capacitor10is determined.

It is preferable, based on the statistical view, that immediately before the luminous flux rises sharply, in accordance with the state of the discharge lamp6, the emission acceleration control be shifted from area A to area B. The shifting condition is defined as VC≧E1and Vs≧E2. That is, “VC≧E1” means that, in the first area A, the capacitor10is charged using a specific time constant so that the voltage is increased. Thereafter, a specific time period or longer elapses. “Vs≧E2” means that the lamp voltage VL has been increased and is equal to or higher than the voltage represented by E2. When these two conditions are established, the emission accelerating control is shifted to the process for increasing the rate at which the supplied power is reduced.

For example, for a discharge lamp for which the initial lamp voltage at the lighting time is high, the supply of power is continued in the first area A for at least a specific period of time. For a discharge lamp for which the initial lamp voltage at the lighting time is low, while taking into account the delay in the rise of the luminous flux, the supply of power in the first area A is continued, even after a specific time period has elapsed, until the lamp voltage VL reaches and corresponds to the voltage represented by E2. Therefore, the affect produced by the variance in the characteristic of the discharge lamp6can be suppressed. As described above, when the terminal voltage VC of the capacitor10is equal to or higher than the threshold value (E1), and the lamp voltage VL is equal to or higher than the threshold value (corresponds to E2), preferably the emission acceleration control is shifted from area A to area B.

In area B, while taking the sharp rise in the luminous flux into account, the current I1of the constant voltage source17and the current I2that depends on the level of the lamp voltage VL are supplied to the capacitor10to increase the rate at which the voltage VC rises. That is, when VC<E3is established, the current I1, as well as in area A, is supplied to the capacitor10. To supply the current I2, the voltage Vs is applied to the NPN transistor35, through the amplifier33and the operating amplifier34, the collector current is returned by the current mirror circuit30, and the collector current of the PNP transistor39is supplied through the diode42to the capacitor10(as the Vs rise rate is increased, the current I2is also increased). The outputs of the comparators43,44and45are all defined as H (high) impedances since Vs>E2, E1<VC and VC<E4are established.

During the period wherein VC<E3, the output of the comparator46in the circuit unit32is defined as the H impedance, and when VC=E3is established, the output level goes to the L (low) signal.

Since in the first half of area B the capacitor10is charged by using two currents, I1and I2, the voltage VC is increased sharply, and the power supplied to the discharge lamp6is reduced quickly. Therefore, if this control state is maintained in the last half of area B, there will be too great a reduction in the power supplied, and the luminous flux will fall.

Therefore, it is preferable that area B be further divided into smaller segments, and that the current I2be changed in each segment, so that the rate at which the supplied power is reduced can be precisely controlled in area B.

In this embodiment, after VC=E3is established (in the last half of area B), the value of the current I2is reduced by the comparator46of the circuit unit32(a current sink).

The time when the emission acceleration control is shifted from area B to area C is determined in accordance with the condition VC=E4. That is, when the voltage VC is equal to or higher than the threshold value (E4), the emission acceleration control is shifted from area B to area C.

In area C, since the control must be performed to maintain the constant lamp voltage VL at substantially a constant level and to thermally stabilize the discharge lamp6, the supply of the current I2to the capacitor10is inhibited. That is, since VC>E4is established, the signal output by the comparator44of the circuit unit31goes to level L, and the supply of the current I2to the capacitor10is halted.

Further, the L signal is output by the comparator27of the circuit unit28, and the NPN transistor24is turned off. Then, the current I1, from the constant voltage source17, is supplied through the resistors19and20to the capacitor10(the time constant is increased), and the VC rising rate in area C is smaller than the VC rising rate in area A. This control process is performed because the supplied power is gradually reduced to shift the discharge lamp6to the steady state. For example, but not by way of limitation, when the same power reduction rate as in area A is set for area C (the time constant is the same), undershoot of the luminous flux will occur, and such a phenomenon must be avoided. Since the supply of the current I2is halted in area C, the current I1is reduced and the charging of the capacitor10is performed.

As described above, among the three area segments of the control area, in the second area B and further, in the middle of the period of the transition to the steady state, the current I1and the current I2are supplied to the capacitor10. In the first area A, at the start of the period of transition to the steady state, and in the third area C, at the end of the period of transition to the steady state, only the current I1is supplied to the capacitor10. That is, in areas A and C, it is preferable that the rate at which the terminal voltage VC of the capacitor10is reduced be low, so as to gradually reduce the rate at which the power is supplied.

In this embodiment, three control area segments have been employed for the power control provided during the transition period; however, the control area may be divided into more segments (it should be noted, however, that preferably the circuit is designed while taking into account a disadvantage, such as the complexity of the circuit structure). However, the present invention is not limited thereto, and equivalents as would be known by those of ordinary skill in the art may be substituted therefore.

For the restarting of the discharge lamp6, two cases apply: the case (i.e., cold start) wherein the discharge lamp6is cool when lighted, since a comparatively long period has elapsed since it was last lighted, and a case (i.e., hot start) when the discharge lamp6is lighted while it is still comparatively warm because a light-off period (the elapsed time following the immediately preceding turn-off time) is short.

In the second case, when the same power is supplied to the discharge lamp6, overshoot of the luminous flux or deterioration of the luminous flux occurs because excessive power is supplied. Therefore, it is preferable that the initial power supplied to the discharge lamp6be designated in accordance with the length of the period during which the discharge lamp is off. An exemplary, non-limiting detection method can be a method whereby, while the discharge lamp is on, the capacitor10is fully charged and when the discharge lamp is turned off in accordance with a turn-off instruction, discharging of the capacitor10begins. When only a small charge remains on the capacitor10at the next start time, this means that a long period has elapsed, and in this case, only the terminal voltage of the capacitor10need be detected.

With the configuration shown inFIG. 4, the period during which the discharge lamp6is in the off state is detected by using the discharging path from the capacitor10, while taking into account the fact that when the lighting of the discharge lamp6is started, the charging path is formed to supply the current I1to the capacitor10. That is, the discharging path from the capacitor10is formed in the direction opposite to that of the charging path when the discharge lamp6is turned off, or when the supply of power to the lighting circuit is halted. Therefore, the discharge time constant defined for the capacitor10is greater than the charging time constant for the capacitor10, so that the counting means for the light off period can be provided.

When the discharge lamp6is turned off, the Eref of the constant voltage source17becomes zero, and the discharging of the capacitor10is performed along the path opposite the path for charging the current I1, and as time elapses, the voltage VC is lowered. For a hot start when the light-off period is short, the lighting is initiated under a condition wherein the voltage VC is slightly lower than the level in the fully charged state, so that the power supplied at the initial lighting time can be suppressed. For a cold start, the lighting is initiated at VC=0. As explained while referring toFIG. 5, power control is provided in accordance with whether the area is A, B or C. When the light-off period is shorter than the period required for a cold start, the power supplied at the lighting start time is controlled based on the value of the voltage VC that is consonant with the charge remaining on the capacitor10.

The discharge time constant for the capacitor10should be set so it is greater than the charge time constant. Otherwise the discharging will be performed too fast, and for detecting the light-off period, the discharge time constant will not be useful. Therefore, the resistances are changed by using the circuit units23and28. That is, when the discharge lamp6is turned off, the NPN transistors21and24are in the off state, and the discharge time constant is determined by the total value (about several hundred kilos to several mega Ω) of the resistances of the three resistors18to20, which are connected in series. So long as the output impedance of the constant voltage source17affects the discharging only to the degree equivalent to an error, there is no problem with the discharging path. When the effect is more than an error, a resistor (having a resistance of about several tens to several kilo Ω) can be provided parallel to the constant voltage source17and discharging through this resistor can be performed.

As discussed above, according to the first aspect of the invention, the related art concept of the control line need not be employed to control power supplied to a discharge lamp during the transition period. Thus, the circuit structure can be simplified and the multiplicity of usages is available. Further, when the present invention is applied for a lighting circuit for a discharge lamp that contains no mercury or only a small amount of mercury, the rate at which the power supplied is reduced can be controlled in accordance with the period and the lamp voltage, so that the starting period can be reduced and stabilized.

According to the second aspect of the invention, the control area is divided into multiple segments, and the change in the power supplied to the discharge lamp (the reduction rate) can be determined for each segment.

According to the third aspect of the invention, the rate at which the terminal voltage of the capacitor is increased is reduced in the first and the third areas, so that the rate at which the power supplied is gradually lowered can be reduced to prevent a rapid drop in the power supplied.

According to the fourth aspect of the invention, the process can easily be performed for determining the condition when the control is shifted from one control area segment to another.

According to the fifth aspect of the invention, the power control can be provided in accordance with variances in the characteristics of the discharge lamp, while taking into account the rise in the lamp voltage and the time that has elapsed since the lighting of the discharge lamp was started.

According to the sixth aspect of the invention, in the third area, since the rate is reduced at which the power supplied is lowered, a discharge lamp can be smoothly shifted to the steady state.

According to the seventh aspect of the invention, the rate at which the power supplied is lowered can be delicately controlled in the second area.

According to the eighth aspect of the invention, for the capacitor10, a discharging path separate from a charging path need not be employed to detect the period a discharge lamp has been off (only the time constant is changed for the same path). Therefore, the circuit structure is simplified, and the costs can be effectively reduced.