JP4049164B2 - Method for manufacturing plasma generating power supply device - Google Patents

Description

  The present invention relates to a method for manufacturing a plasma generating power supply device such as an ozone generator or a laser oscillator.

Conventionally, a plasma generating power supply device is used for an ozone generator, a laser oscillator, or the like.
FIG. 12 is a power supply circuit diagram of a conventional plasma generating power supply device for an ozone generator (see, for example, Non-Patent Document 1).
In FIG. 12, 1 is an AC input power source, 2 is a rectifier, 3 is an inverter, 4 is a transformer (transformer), and 5 is a gas region serving as a discharge space via a dielectric between a pair of opposed electrodes. A discharge load 6 in which plasma is generated when the gas in the discharge space is excited, and 6 is a parallel inductor for power factor improvement connected in parallel to the discharge load 5.

Next, the operation will be described.
The commercial AC voltage of the input power supply 1 is converted to DC by a rectifier, and further converted to AC voltage of a specified frequency by an inverter 3. Further, the voltage is raised to the voltage at which discharge starts by the transformer 4, and a high voltage is applied to the discharge load 5. The applied high voltage causes a discharge in the discharge load 5, and the gas particles are excited by this discharge.
Here, when a discharge load in which a dielectric is inserted between the discharge electrodes is used, it is known that the discharge load 5 functions electrically as a capacitor and the phase of current advances with respect to voltage. For this reason, the power factor represented by the ratio of the apparent power and the active power is low, and in order to input energy to the discharge load 5, it is necessary to pass a current more than necessary.

Therefore, since the elements constituting the transformer 4 and the inverter 3 require specifications that can withstand the above current values, an increase in the size of the power supply device and an increase in device cost are inevitable.
The parallel inductor 6 is connected in parallel with the discharge load 5 as a phase delay element in order to compensate the advance of the current phase in the discharge load with respect to the voltage. If the current phase advance in the discharge load 5 and the current phase delay by the parallel inductor 6 are set to be equal, the phase of the current and voltage supplied from the power supply device match, and the discharge current 5 can be efficiently used with the smallest current. Can be powered. If each element is an ideal element, the power factor at this time is 100%, which is a state called resonance.

In the conventional plasma generating power source, the power factor is improved by connecting the parallel inductor 6 in parallel with the discharge load 5 in this way, and a small and inexpensive power source device can be configured using a small capacity power source element. ing.
12 shows the case where a parallel inductor is connected to the secondary side of the transformer 4. However, the same effect can be obtained by connecting a parallel inductor to the primary side of the transformer 4 as shown in FIG. . However, in this case, an element having a low withstand voltage can be used, but the power factor of the transformer is not improved, and therefore a transformer having a capacity larger than necessary is required.

  FIG. 14 is an equivalent circuit of the discharge load 5 in which a dielectric is interposed between electrodes such as an ozone generator. In FIG. 14, reference numeral 51 denotes a dielectric capacitance interposed between the electrodes, and has a capacitance value C1. 52 is the capacitance of the gas region and has a capacitance value C2. Reference numeral 53 denotes a Zener diode equivalently showing a plasma load portion having non-linearity due to generation and extinction of plasma.

The resistance value of the plasma load 53 is infinite when it is less than the Zener voltage Vz, and no current flows. That is, the circuit is in a non-discharge state. However, when the voltage across the element 53 reaches the zener voltage Vz, the element becomes conductive and the circuit is discharged.
For this reason, in the non-discharged state, the discharge load 5 is a capacitive load having a value C represented by the equation (3) in which the value C1 of the dielectric capacitance 51 and the value C2 of the gas capacitance 52 are coupled in series. However, it changes to a capacitive load having a capacitance value C1 alone during discharge.
C = {C1 × C2 / (C1 + C2)} (3)

  The conventional ozone generator is designed such that the capacitance value C1 of the dielectric capacitance 51 is sufficiently larger than the capacitance value C2 of the gas capacitance 52. That is, the gap in the gas region where discharge occurs is as wide as several mm. For this reason, the load capacity value C at the time of non-discharge represented by Expression (3) is C≈C2, and has an extremely small capacity component. Further, the load capacity value at the time of discharge is C1, and the load capacity value changes greatly at the time of discharge / non-discharge. However, at the time of non-discharge, the capacitive component of the load is very small as described above. Therefore, even if the current phase is advanced and the power factor is bad, the reactive power itself is small, so that the capacity of the power source is not significantly increased. For this reason, when the capacitance value C1 of the dielectric capacitance 51 is sufficiently larger than the capacitance value C2 of the gas capacitance 52 as in the conventional ozone generator, the load capacitance value at the time of discharge is set. An inductor that satisfies the resonance condition was selected in accordance with C1.

"Ozonizer Handbook" (Corona, June 15, 1960, 227 pages, Fig. 2.63)

  The conventional plasma generating power supply device is configured to compensate the capacitance of the discharge load 5 with one type of inductor for the discharge load 5. In the conventional example using an ozone generator as an example, the capacitance value C2 of the gas capacitance 52 is sufficiently smaller than the capacitance value C1 of the dielectric capacitance 51. The power factor could be improved by selecting an inductor to compensate. However, most recent ozone generators have a gas region with a gap (hereinafter referred to as a discharge gap length) of 1 mm or less in order to improve the performance. Therefore, the capacitance value C2 of the gas capacitance 52 increases to a level that cannot be ignored as compared with the capacitance value C1 of the dielectric capacitance 51, and depending on the device, there is a case where C1≈C2 or C1 <C2. Exists. In this case, not only the capacitance value of the discharge load 5 changes depending on the occurrence of discharge, but also has a large capacitance component even during non-discharge. Therefore, the reactive power at the time of non-discharge, which has not been a problem in the past, has increased, and the power factor compensation at the time of non-resonance has not been made. No longer. This makes the device larger and more expensive. Thus, there are problems to be solved in the conventional plasma generating power supply device.

The present invention has been made in order to solve the above-described problems. The discharge gap length in the gas region is 1 mm or less, and the capacitance value in the gas region is ignored compared to the capacitance value of the dielectric. It is an object of the present invention to provide a method for manufacturing a power supply device for plasma generation that can perform power factor compensation for a discharge load that cannot be performed regardless of whether or not a discharge occurs, and that is therefore small and inexpensive.

In the method for manufacturing a plasma generating power supply device of the present invention, a gas region serving as a discharge space is formed between a pair of electrodes arranged opposite to each other via a dielectric, and an electric field generated by an alternating high voltage applied between the electrodes. In the plasma generating power supply apparatus for supplying AC power via a transformer to a discharge load that excites the gas in the discharge space to generate plasma, the discharge gap length of the gas region is 1 mm or less, and the gas If the capacitance value C2 of the region is an electrostatic capacitance value large enough not negligible compared to C1 of the dielectric, as well as configured to have an inductance in parallel or in series with respect to the discharge load, The inductance value L on the secondary side of the transformer is determined by the capacitance value C1 of the discharge load during the discharge period. Between the value and the value determined by the capacitance value C3 = (C1 × C2) / (C1 + C2) of the discharge load in the non-discharge period, and set so as to satisfy the following formula (1) It is a thing.
1 / {C1 × (2πf) ² } ≦ L ≦ 1 / {C3 × (2πf) ² } (1)
Where f: frequency of AC voltage applied between both electrodes

As described above, according to the present invention, the inductance is configured in parallel or in series with the discharge load, and the inductance value L is expressed by the equation (1) as follows: Therefore, the discharge gap length of the gas region is 1 mm or less, and the discharge load is such that the capacitance value of the gas region is not negligible compared to the capacitance value of the dielectric. Thus, power factor compensation can be performed stably regardless of whether or not discharge is generated, and as a result, a small and inexpensive plasma generating power supply device can be manufactured.

Embodiment 1 FIG.
Embodiment 1 of the present invention will be described below with reference to the drawings.
FIG. 1 is a circuit diagram showing a plasma generating power supply apparatus according to Embodiment 1 of the present invention. In FIG. 1, 1 is an AC power source for input, 2 is a rectifier, 31 is an inverter, and 4 is a transformer (transformer). Reference numeral 5 denotes a discharge load in which a gas region serving as a discharge space is formed between a pair of opposed electrodes via a dielectric, and the gas in the discharge space is excited to generate plasma. A dielectric capacitance 51 The gas capacitance 52 and the Zener diode 53 can be equivalently shown in FIG. Reference numeral 61 denotes a parallel inductor for power factor improvement which is connected in parallel to the discharge load 5 and the secondary winding of the transformer 4 and has an inductance Lp1. Although not specified in the prior art, when the circuit configuration is as described above, the inverter 31 uses a constant current control type inverter whose output current waveform is a rectangular wave.

  Such a plasma generation power supply device is applied as, for example, a power supply for an ozone generator, but is not limited to this. ), And can also be applied to devices such as light sources using electric discharge. This also applies to the embodiments described below.

Next, the operation will be described.
The commercial AC voltage of the input power source 1 is converted into a direct current by the rectifier 2 and further converted into an alternating current having a specified frequency by the inverter 31. In this case, the inverter 31 uses a constant current control inverter. The output voltage from the inverter 31 is boosted by the transformer 4 and then divided into the dielectric capacitance 51 and the gas capacitance 52 according to the inverse ratio of the respective capacitance values. Then, when the voltage divided by the gas capacitance 52 reaches the zener voltage Vz, the discharge load 5 generates a discharge.

In a general ozonizer, an AC voltage having a frequency of about several tens of kHz from a commercial frequency is applied. In such a frequency range, a discharge period and a non-discharge period appear twice in one cycle, respectively. Thus, a parallelogram V (voltage) -Q (charge) Lissajous waveform that is substantially biaxially symmetric is obtained. In FIG. 2, the horizontal axis V is the voltage at both ends of the discharge load 5, the vertical axis Q is the charge at both ends of the discharge load 5, points B and D are the discharge start points, and points A and C are the discharge end points. is there. Here, the intercept of the V-axis at Q = 0 is a state in which no electric charge is induced in each capacitive element represented by the equivalent circuit of the discharge load, so that the gas region is being discharged and both ends of the dielectric. Since no voltage is generated, it is represented by the discharge sustaining voltage V ^* in the discharge space, and V = V ^* and −V ^* . The discharge sustaining voltage V ^* is a temporal / spatial average value of the voltage generated in the discharge space during the discharge period, but actually, the discharge is generated randomly in time and space. Therefore, a steady discharge can be assumed. Therefore, the sustaining voltage V ^* is substantially equal to the discharge start voltage in the gas region, that is, the Zener voltage Vz, and has a relationship of V ^* ≈Vz.
In FIG. 2, tan α represents the capacitance value of the discharge load 5 during the discharge period. During the discharge period, the gas capacitance 52 (capacitance value C2) is short-circuited, and the dielectric capacitance 51 (capacitance value). Since only C1) contributes,
tan α = C1 (4)
It becomes.
Furthermore, a region having an inclination represented by the angle β is a non-discharge period. Since the equivalent circuit at the time of non-discharging ignores the stray capacitance of the circuit, the dielectric capacitance 51 and the gas capacitance 52 are connected in series.
tan β = C1 × C2 / (C1 + C2) (5)
It is represented by

Here, the alternate long and short dash line connecting points A and C in FIG. 2 passes through the origin because the Lissajous waveform is biaxially symmetric. Since this is a straight line connecting the start point of the non-discharge period and the end point of the discharge period, it represents the average capacitance of the discharge load 5 evaluated including the non-discharge period and the discharge period. Become. Assuming that the inclination angle of this straight line is γ, the maximum charge amount Q _{max at} point C in the figure is tan α = C1.
Q _max = (V _op −V ^* ) × tan α
= C1 × (V _op −V ^* ) (6)
It can be expressed as. Therefore, the inclination angle γ of the straight line indicated by the alternate long and short dash line is as shown in FIG.
tan γ = Q _max / V _op = C1 × (1−V ^* / V _op ) (7)
Given in.

Here, FIG. 3 shows the state of the discharge load 5 at the end of discharge (V = V _op ). When the voltage divided into the gas region reaches the zener voltage Vz, the gas is broken down, so that the capacitance 52 in the gas region is short-circuited. At this time, if the Zener diode has only the non-linear resistance component R, only the dielectric capacitance 51 contributes as the capacitance component of the discharge load 5 as viewed from the power source. That is, the discharge load 5 can be regarded as an element in which the capacitance 51 and the resistor R of the Zener diode are connected in series.

When the apparent capacity component of the discharge load 5 as viewed from the power source side is evaluated at the end of the discharge, the charge Q stored in the discharge load 5 is expressed by Q = Q _max = C1 × (V _op from Vz≈V ^*. −V ^* ), and at this time, the voltage V _op is applied to the discharge load 5, so the capacitance value C of the discharge load is
C = Q _max / V _op = C1 × (1−V ^* / V _op ) (8)
It becomes. This value is equal to the value of the average capacitance (tan γ) of the discharge load including the non-discharge period and the discharge period described above. That is, from the power source side, the discharge load 5 appears as if it is a capacitance component having the capacitance value C represented by the equation (8) throughout one cycle. Therefore, in order to efficiently supply power to the discharge load 5, an inductor having an inductance sufficient to cancel the capacitance component C of the discharge load viewed from the power source side expressed by the following equation (9) may be added. good.
L = 1 / [C × (2πf) ² ] (9)
Where L: inductance of the inductor to be added [H]
C: capacitance value [F] given by C1 × (1−V ^* / V _op )
C1: Capacitance value of dielectric [F]
V ^* : discharge sustaining voltage [V] in the discharge space
V _op : Applied voltage peak value [V]
f: Frequency of AC voltage applied between both electrodes [Hz]

  From the above, in FIG. 1, if the inductance Lp1 of the parallel inductor 61 connected in parallel to the discharge load 5 is set to L which satisfies the equation (9), the capacitance in the gas region A high power factor can be maintained even for a discharge load whose value C2 is not negligible compared to the capacitance value C1 of the dielectric. As an example, the resonance frequency f and the parallel inductor 61 in the case where the dielectric capacitance value C1 and the gas region capacitance value C2 have discharge loads with C1 = 10.9 nF and C2 = 8.4 nF, respectively. FIG. 4 shows the result of examining the relationship of the inductance Lp1. From FIG. 4, it can be seen that a resonance state is obtained by an inductor having an inductance very close to the calculated value of Lp1 given by Expression (9). In this case, the power factor of the discharge load 5 in the state where the parallel inductor 61 is not inserted is 30% or less. However, by connecting the inductor 61 for power factor compensation to the discharge load 5 in parallel, the transformer 4 is included. The power factor of the discharge load 5 can be improved to 90% or more.

FIG. 5 shows a power factor improving inductor 61 having an inductance Lp1 = 0.16H connected in parallel to the discharge load 5 in an ozonizer having a discharge load 5 with a dielectric capacitance value C1 of 49.5 nF. In this case, the relationship between the resonant frequency f and the applied voltage peak value V _op is shown. Also from this figure, the calculated resonance frequency given by equation (9) and the experimentally obtained resonance frequency fall within the range of ± 2%, and the resonance condition can be determined with very high accuracy by equation (9). It suggests that it is possible to predict.

In the electrical design of the ozonizer, first, the discharge power W input to the apparatus is determined. Discharge power W is given by the following equation.
W = 4 · f · C1 · V ^* × {V _op − (1 + C2 / C1) · V ^* } (10)
It is. Among these, physical quantities other than V _op are obvious if the electrode material and shape, and the operating conditions such as gas pressure are determined. Therefore, the applied voltage peak value V _op for obtaining the desired discharge power W is obtained by the equation (10). If V _op is determined, since C1 and V ^* are also known, the capacity component C of the discharge load 5 as seen from the power source can also be obtained by Expression (8). The inductor for power factor improvement can be easily designed by (9).

  As described above, according to the first embodiment, the inductance of the parallel inductor 61 connected in parallel to the discharge load 5 is set so as to satisfy Expression (9). There is an effect that the rate improvement degree can be maintained high.

Embodiment 2. FIG.
FIG. 6 is a circuit diagram showing a plasma generating power supply apparatus according to Embodiment 2 of the present invention. In FIG. 6, reference numeral 62 denotes a parallel inductor for power factor improvement having an inductance value Lp2 connected in parallel to the discharge load 5 and the secondary winding of the transformer 4, and the basic circuit configuration is the same as that of the first embodiment. It is exactly the same. Although not specified in the prior art, when the circuit configuration is as described above, the inverter 31 uses a constant current control type inverter whose output current waveform is a rectangular wave, as in the first embodiment. Note that the same or similar elements as those of the first embodiment are denoted by the same reference numerals and description thereof is omitted.

Next, the operation will be described.
In the second embodiment, as shown in FIG. 6, the inductance value Lp2 of the parallel inductor 62 connected in parallel to the discharge load 5 is set so as to satisfy the following equation.
1 / {C1 × (2πf) ² } ≦ Lp2 ≦ 1 / {C3 × (2πf) ² } (11)
Here, C1: capacitance value [F] of the dielectric
f: Frequency of AC voltage applied between both electrodes [Hz]
C3: capacitance value [F] given by (C1 × C2) / (C1 + C2)
C2: Capacitance value of gas region [F]
It is. C3 is a series composite capacitance of the dielectric capacitance and the gas region capacitance, and is a capacitance component of the discharge load 5 during non-discharge as viewed from the power source side.

In the first embodiment, since a state very close to the resonance condition can be reproduced, it is possible to input power to the discharge load 5 with very high efficiency, and the required current capacity of the inverter 31 can be minimized. However, the operation at the resonance point is generally sensitive to changes in physical quantities such as load capacitance. Taking an ozonizer as an example, the capacity of the discharge load 5 may change due to dielectric breakdown of the dielectric. (In this case, the capacitance of the load 5 decreases.) For this reason, it can be considered that the resonance point is actually deliberately shifted. At this time, if the inductance of the inductor 62 is selected within a range that satisfies the equation (11), as can be seen from the Lissajous waveform of FIG.
C3 <C <C1 (12)
(Where C is the capacitance value given by C1 × (1-V ^* / V _op ))
Therefore, it is possible to set the inductance of the inductor 62 at a position slightly removed from the resonance point. Although the degree of power factor improvement does not reach that of the first embodiment, the degree of power factor improvement can be stably maintained high with respect to the change in the discharge load 5.

Furthermore, the capacity component C ′ of the discharge load 5 is C <C ′ <C1 (13)
(Where C is the capacitance value given by C1 × (1-V ^* / V _op ))
If the inductor for power factor improvement is designed to be in the range of, even if the capacitance of the discharge load is reduced as described above, the load capacitance component is estimated to be larger than the value satisfying the resonance condition in advance. The power factor can be prevented from deteriorating significantly. In this case, if the capacity decrease is small, the power factor at that time may be improved as compared with the design time.

As described above, according to the second embodiment, the inductance Lp2 of the parallel inductor 62 connected in parallel to the discharge load 5 is set so as to satisfy the expression (11). Power factor improvement degree can be maintained high.
Furthermore, if the inductance of the inductor 62 is determined on the assumption that the capacitance component C ′ of the discharge load 5 is within the range satisfying the expression (13), the force can be reduced even if the capacitance of the discharge load decreases due to dielectric breakdown or the like. It is possible to avoid the rate from becoming extremely worse, and to stably maintain a high power factor improvement degree.

Embodiment 3 FIG.
FIG. 7 is a circuit diagram showing a plasma generating power supply device according to Embodiment 3 of the present invention. In FIG. 7, 7 is a series inductor for power factor improvement, which is connected in series with the discharge load 5 and the secondary winding of the transformer 4 and has an inductance Ls1. Although not specified in the prior art, in the case of the circuit configuration as described above, in this embodiment, the inverter 32 uses a constant voltage control type inverter whose output voltage waveform is a rectangular wave. Note that the same or similar elements as those of the above-described embodiment are denoted by the same reference numerals and description thereof is omitted.

  In FIG. 7, when the constant voltage control type inverter 32 as described above is used, the inductance (Ls1) of the series inductor 7 connected in series to the discharge load 5 also satisfies the expression (9). In this case, a high power factor can be maintained even for a discharge load in which the capacitance value C2 in the gas region is not negligible compared to the capacitance value C1 of the dielectric. The same effect can be obtained.

  Further, when the inductance Ls2 of the series inductor 7 is selected so as to satisfy the expression (11), the power factor improvement degree is slightly deteriorated, but the power factor is more stable against the change of the discharge load 5. It is possible to keep the rate improvement degree high.

Embodiment 4 FIG.
FIG. 8 is a circuit diagram showing a plasma generating power supply apparatus according to Embodiment 4 of the present invention. In the fourth embodiment, a parallel inductor 63 is connected in parallel with the primary side winding of the transformer 4. Note that the same or similar elements as those of the first embodiment are denoted by the same reference numerals and description thereof is omitted.

In FIG. 8, the inductance Lp3 of the parallel inductor 63 connected in parallel with the primary winding of the transformer 4 is the parallel inductor 61 connected to the secondary side of the transformer 4 shown in the first and second embodiments. When the turns ratio of the transformer 4 (secondary turns / primary turns) is m, with respect to the inductances Lp1 and Lp2 of 62,
Lp3 = Lp1 / m ² (14)
Lp3 = Lp2 / m ² (15)
It is comprised so that either of these may be satisfied. In this way, the same LC parallel circuit as that shown in the first or second embodiment is equivalently obtained, and the same effect can be obtained. That is, the transformer 4 can be configured to have an inductance satisfying the formula (1) or the formula (2) in parallel with the discharge load 5 on the secondary side.

Embodiment 5. FIG.
FIG. 9 is a circuit diagram showing a plasma generating power supply apparatus according to Embodiment 5 of the present invention. In the fifth embodiment, a series inductor 71 is connected in series with the primary side winding of the transformer 4. Note that the same or similar elements as those of the third embodiment are denoted by the same reference numerals and description thereof is omitted.

In FIG. 9, the inductance Ls3 of the series inductor 71 connected in series with the primary winding of the transformer 4 is the inductance of the series inductor 7 connected to the secondary side of the transformer 4 shown in the third embodiment. When the turns ratio of the transformer 4 is m with respect to Ls1 or Ls2,
Ls3 = Ls1 / m ² (16)
Ls3 = Ls2 / m ² (17)
It is comprised so that either of these may be satisfied. In this way, the same LC parallel circuit as that shown in the third embodiment is equivalently obtained, and the same effect can be obtained. That is, the transformer 4 can be configured to have an inductance that satisfies the formula (1) or the formula (2) in series with the discharge load 5 on the secondary side.

Embodiment 6 FIG.
FIG. 10 is a circuit diagram showing a plasma generating power supply device according to Embodiment 6 of the present invention. In FIG. 10, reference numeral 64 denotes a parallel inductor equivalently connected in parallel to the primary side winding of the transformer 4, which corresponds to the exciting inductance of the transformer 4. In addition, the same code | symbol is attached | subjected about the element equivalent or the same as Embodiment 1, and description is abbreviate | omitted.

Next, the operation will be described.
In the first embodiment, the parallel inductor 61 is connected in parallel with the secondary winding of the transformer 4. However, the same effect can be obtained by using the exciting inductance of the transformer 4 instead of the parallel inductor 61. To do. In this case, since the power factor is improved on the primary side of the transformer 4, the inductance Lp4 of the parallel inductor 64 is parallel inductors 61 and 62 connected to the secondary side of the transformer 4 shown in the first and second embodiments. When the turns ratio of the transformer 4 is m with respect to the inductances Lp1 and Lp2 of
Lp4 = Lp1 / m ² (18)
Lp4 = Lp2 / m ² (19)
It is comprised so that either of these may be satisfied.
Specifically, the value of the excitation inductance is adjusted by increasing / decreasing the length of the gap between the primary iron core and the secondary iron core of the transformer (the larger the gap, the smaller the magnetizing inductance). It is set to a predetermined value that satisfies either one.

  In this way, the same LC parallel circuit as that shown in the first or second embodiment is equivalently obtained, and the same effect can be obtained. That is, the transformer 4 can be configured to have an inductance satisfying the formula (1) or the formula (2) in parallel with the discharge load 5 on the secondary side.

  Furthermore, in the sixth embodiment, the transformer 4 is designed using the exciting inductance of the transformer 4 so that the exciting inductance Lp4 satisfies either of the equations (18) and (19) in advance. Has the same role as the parallel inductors 61 and 62 of the first or second embodiment, so that it is not necessary to newly connect a parallel inductor, so that a cheaper device can be provided.

Embodiment 7 FIG.
FIG. 11 is a circuit diagram showing a plasma generating power supply apparatus according to Embodiment 7 of the present invention. In FIG. 11, 72 is a series inductor equivalently connected in series to the primary side winding of the transformer 4, and corresponds to the leakage inductance of the transformer 4. In addition, the same code | symbol is attached | subjected about the element equivalent or the same as Embodiment 3, and description is abbreviate | omitted.

Next, the operation will be described.
In the third embodiment, the series inductor 7 is connected in series with the secondary side winding of the transformer 4, but the same effect can be obtained by using the leakage inductance of the transformer 4 instead of the series inductor 7. To do. In this case, since the power factor is improved on the primary side of the transformer 4, the inductance Ls4 of the series inductor 72 is the inductance Ls1 of the series inductor 7 connected to the secondary side of the transformer 4 shown in the third embodiment. Or when the turns ratio of the transformer 4 is m with respect to Ls2,
Ls4 = Ls1 / m ² (20)
Ls4 = Ls2 / m ² (21)
It is comprised so that either of these may be satisfied.
Specifically, the value of the leakage inductance is adjusted by increasing or decreasing the amount (cross-sectional area) of the iron core of the transformer (the larger the cross-sectional area, the larger the leakage inductance), and a predetermined value that satisfies one of the above formulas Set to.

  In this way, the same LC parallel circuit as that shown in the third embodiment is equivalently obtained, and the same effect can be obtained. That is, the transformer 4 can be configured to have an inductance that satisfies the formula (1) or the formula (2) in series with the discharge load 5 on the secondary side.

Further, in the seventh embodiment, the leakage inductance of the transformer 4 is used, and the transformer 4 is designed in advance so that the leakage inductance Ls4 satisfies either of the expressions (20) and (21). Has the same role as the series inductor 7 of the third embodiment, so that it is not necessary to newly connect a series inductor, so that a cheaper device can be provided.

It is a circuit diagram which shows the power supply device for plasma generation by Embodiment 1 of this invention. It is a figure which shows a V (voltage) -Q (electric charge) Lissajous waveform when an ozonizer is taken as an example. It is a figure explaining the equivalent circuit of the ozonizer at the time of completion | finish of discharge. It is a figure which shows the relationship between the resonant frequency and the inductance value of the inductor to add. It is a figure which shows the relationship between a resonant frequency and an applied voltage peak value. It is a circuit diagram which shows the power supply device for plasma generation by Embodiment 2 of this invention. It is a circuit diagram which shows the power supply device for plasma generation by Embodiment 3 of this invention. It is a circuit diagram which shows the power supply device for plasma generation by Embodiment 4 of this invention. It is a circuit diagram which shows the power supply device for plasma generation by Embodiment 5 of this invention. It is a circuit diagram which shows the power supply device for plasma generation by Embodiment 6 of this invention. It is a circuit diagram which shows the power supply device for plasma generation by Embodiment 7 of this invention. It is a circuit diagram which shows the conventional power supply device for plasma generation. It is a circuit diagram which shows another conventional power supply apparatus for plasma generation. It is a figure which shows the equivalent circuit of a discharge load.

Explanation of symbols

  1 AC power supply, 2 rectifier, 3, 31, 32 inverter, 4 transformer, 5 discharge load, 51 dielectric capacitance, 52 gas capacitance, 53 Zener diode, 6, 61, 62, 63, 64 parallel inductor, 7, 71, 72 Series inductor.

Claims (5)

A gas region serving as a discharge space is formed between a pair of opposed electrodes via a dielectric, and a plasma is generated by exciting the gas in the discharge space by an electric field generated by an alternating high voltage applied between the electrodes. In a plasma generating power supply apparatus that supplies alternating current power to a discharge load through a transformer, a discharge gap length of the gas region is 1 mm or less, and a capacitance value C2 of the gas region is a static value of the dielectric. In the case where the magnitude is not negligible compared to the capacitance value C1, the inductor is configured to have an inductance in parallel or in series with the discharge load, and the inductance value is set on the secondary side of the transformer. The inductance value L is determined by the capacitance value C1 of the discharge load during the discharge period, and the capacitance of the discharge load during the non-discharge period. C3 = (C1 × C2) / A value determined by (C1 + C2), and a method for manufacturing a plasma generating power supply device, characterized in that the value is set so as to satisfy the following formula (1) .
1 / {C1 × (2πf) ² } ≦ L ≦ 1 / {C3 × (2πf) ² } (1)
Where f: frequency of AC voltage applied between both electrodes The secondary side of the transformer, the claims as well as the inductor is connected in parallel or series with the discharge load, the inductance of the inductor, characterized by being set to a value L of the inductance that satisfies the equation (1) 1 Symbol placement of a method of manufacturing a plasma generation power source device. When the inductance represented by the formula (1 ) is L and the turns ratio of the transformer is m, an inductor is connected in parallel or in series with the discharge load on the primary side of the transformer, and the inductance value of the inductor is set as follows. the process according to claim 1 Symbol placement of the plasma generation power source device is characterized in that set in L / m ^2. The inductance L of the formula (1), when the turns ratio of the transformer and m, transformer magnetizing inductance, claim 1 Symbol placing the plasma generation, characterized in that so as to satisfy L / m ² Method for manufacturing a power supply device for an automobile. The inductance L of the formula (1), when the turns ratio of the transformer and m, transformer leakage inductance, claim 1 Symbol placing the plasma generation, characterized in that so as to satisfy L / m ² Method for manufacturing a power supply device for an automobile.

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