Patent Grant
8232729
The present invention relates to the production of microplasma, and in particular, to a plasma producing apparatus for producing plasma limited in medium gas and a method of plasma production.
Recently, a microplasma jet is drawing attention due to its wide applicability, and has been realized by various power sources and electrode structures. The microplasma is characterized by a minute spatial size. In order to produce and keep plasma in a minute space, the medium density must increases so as to ensure the sufficient collision frequency between electrons/ions and atomic molecules of medium gas (plasma-producing gas). Therefore, the production of microplasma requires medium gas in the vicinity of an atmospheric pressure, i.e., medium gas with a density of about 1018 to 1022 cm−3.
Furthermore, generally, in the case of plasma on a conventional microscale, an electron temperature Te and a gas temperature Tg in the plasma reach almost the thermal equilibrium along with the increase in a working pressure, so that such plasma is called thermal equilibrium plasma. In contrast, in a region of microplasma, which has a size of μm scaled down from several mm, the energy is not transferred sufficiently by the collision between particles because of a shortened duration period τd of medium gas molecules in the plasma, and the non-equilibrium state of Te>>Tg is considered to be obtained as in low-pressure plasma.
Conventionally, a microplasma jet is produced in most cases by an afterglow system using plasma with a temperature thereof decreased. According to the afterglow system, plasma at a relatively high temperature produced inside a quartz pipe through which medium gas flows is pushed by a medium gas stream and blown out from the tip end of the pipe.
For example, according to a system described in Patent Document 1, argon (Ar) gas used as medium gas for producing plasma is allowed to flow into a quartz pipe and is jetted from a jet port. A coil is placed around the quartz pipe and a high-frequency current is induced to flow therethrough, whereby an induction electric field is generated in the quartz pipe. Argon atoms of the argon gas flowing into the quartz pipe are ionized in the induction electric field or magnetic field to become plasma at a high temperature (6,000 to 7,000° C.), and the plasma thus produced is pushed by the flow-in pressure of the argon gas to be jetted to the atmosphere from the jet port at the tip end of the quartz pipe. The jetted plasma generates a microplasma jet without being diffused due to the presence of the atmosphere.
On the other hand, as a system different from those described above, a system as shown in
The LF plasma jet has unusual features in two aspects. First, unlike a plasma jet according to the afterglow system, a plasma jet that extends in an elongated shape and has a large ratio of a length to a diameter (i.e., aspect ratio) is obtained, and the jetting direction is determined in accordance with the direction of a voltage to be applied to the electrodes. More specifically, when the direction of a voltage to be applied to the electrodes is inverted, the jet extends in an opposite direction, i.e., in an upstream direction of gas. Furthermore, according to the high time resolution measurement, columnar discharge is not maintained, and a spherical plasma bullet is moving at a very high speed of 10 km/s, which is about 10,000 times that of a medium gas stream, in synchronization with the power source frequency. Thus, the production mechanism is not directly related to the medium gas stream.
Unlike the afterglow jet, in the plasma jet according to the above system, a medium gas stream is ionized to become plasma, so that the plasma can be radiated directly to an object. Furthermore, in the LF plasma jet, a pulse-shaped plasma bullet is jetted. Therefore, non-equilibrium in terms of time is created, i.e., a thermal non-equilibrium state is created since the energy cannot be transferred to neutral gas at each moment. The thermal non-equilibrium plasma can radiate a high-energy component without raising the temperature of the object.
As described above, according to the LF plasma jet system, a high potential is applied to the electrode 3b, whereby a plasma jet 5 extends in a downstream direction with respect to the medium gas stream. However, it was found that the jetting direction is not determined by the position of the electrode 3b on a high potential side with respect to the electrode 3a on a ground potential side.
More specifically, a plasma jet is produced only due to the presence of the electrode 3b to which a high potential is applied, and the electrode 3a at a ground potential tends to suppress the flow of the jet. On the downstream side in the medium gas stream with respect to the electrode 3b at a high potential, partial discharge occurs between the high potential portion and the ground potential portion present distant from the high potential portion. Furthermore, the discharge produces plasma limited in a medium, which is produced only in the medium gas stream, such as that obtained when the medium gas stream is ionized to become plasma. On the other hand, on the upstream side in the medium gas stream with respect to the electrode 3b at a high potential, discharge occurs due to the short-circuit between electrodes covered with a dielectric barrier, because the interval between the electrode 3b at a high potential and the electrode 3a at a ground potential is small. Unlike partial discharge, the discharge caused by a short-circuit has high power consumption and involves the generation of heat. It was found that the two-electrode system has poor efficiency since such short-circuit discharge occurs.
Furthermore, the discharge mechanism of the LF plasma jet is not known, so that the dischargeable range under various parameters is limited.
Thus, an object of the present invention is to provide a plasma producing apparatus capable of producing plasma limited in medium gas with high energy efficiency stably over a wide range of parameters through a simple configuration, and a method of plasma production.
In order to solve the above problem, a plasma producing apparatus with a first configuration of the present invention, which produces plasma from a medium gas mass in an elongated shape, includes an electric field forming element that forms an electric field in the medium gas mass. The electric field forming element forms an electric field so that partial discharge occurs from the electric field forming element toward both sides in a longitudinal direction of the medium gas mass.
A plasma producing apparatus with a second configuration of the present invention, which produces plasma from a medium gas mass in an elongated shape, includes a single high-potential electrode placed in the medium gas mass, and a voltage applying element that applies a voltage to the high-potential electrode. The voltage applying element applies a voltage, which forms an electric field causing partial discharge from the high-potential electrode toward both sides in a longitudinal direction of the medium gas mass, to the high-potential electrode.
A first method of plasma production of the present invention is for producing plasma from a medium gas mass in an elongated shape by an electric field forming element that forms an electric field in the medium gas mass. The electric field is formed in the medium gas mass by the electric field forming element so that partial discharge occurs from the electric field forming element toward both sides in a longitudinal direction of the medium gas mass.
A second method of plasma production of the present invention is for producing plasma from a medium gas mass in an elongated shape by an electric field forming element that forms an electric field in the medium gas mass. A single high-potential electrode is placed in the medium gas mass, and a voltage, which forms an electric field causing partial discharge from the electric field forming element toward both sides in a longitudinal direction of the medium gas mass, is applied to the high-potential electrode.
In the present specification, the partial discharge refers to a phenomenon in which, when a voltage is applied between electrodes, atmospheric gas between the electrodes is discharged therebetween partially, and does not include the discharge in which the area between the electrodes is short-circuited completely. Such partial discharge occurs when there is a non-uniform electric field distribution, a non-uniform gas distribution with varying breakdown voltages, or the like. For example, when the electrode has a sharp structure instead of a parallel plate structure, an electric field is concentrated at the tip end of the electrode, and the intensity of the electric field increases. If the intensity of the electric field exceeds the breakdown electric field of the atmospheric gas, partial discharge occurs only in this portion.
The use of such partial discharge is based on the finding by the inventors of the present invention regarding the discharge mechanism of an LF plasma jet. More specifically, the discharge mechanism of the LF plasma jet is considered as follows: a streamer corona discharge phenomenon caused by the concentrated intensity of an electric field in the vicinity of a high-voltage electrode occurs along a helium gas flux in the atmosphere or in a glass tube.
In the LF plasma jet producing apparatus and production method of the present invention, an electric field is formed in a medium gas mass in an elongated shape so that partial discharge occurs in a longitudinal direction thereof, whereby plasma can be produced with high energy efficiency stably over a wide range of parameters through a simple configuration.
A plasma producing apparatus of the present invention can take the following various aspects on the basis of the above configuration.
More specifically, the above plasma producing apparatus with the first configuration includes a gas stream generating element that generates a medium gas stream as the medium gas mass, wherein the electric field forming element forms an electric field so that partial discharge occurs from the electric field forming element toward both an upstream side and a downstream side in the medium gas stream.
The above plasma producing apparatus with the first configuration further includes a gas supply member that guides medium gas to the electric field forming element through an internal hollow, wherein the medium gas stream is generated by the gas supply member.
Furthermore, it is preferred that the electric field forming element is capable of forming a strong electric field capable of starting partial discharge in the medium gas mass and a weak electric field capable of maintaining the partial discharge.
The above plasma producing apparatus with the second configuration further includes a gas supply member that guides medium gas to the electric field forming element through an internal hollow, wherein the medium gas stream is generated by the gas supply member.
Furthermore, the gas supply member may be made of a dielectric, and the high-potential electrode may be provided outside of the gas supply member.
Furthermore, the gas supply member may have an opening in a flat plate shape, through which the medium gas is released, and the high-potential electrode may be provided in a flat plate shape on a plate surface of the opening. Alternatively, the gas supply member may have a cylindrical structure, and the high-potential electrode may have a cylindrical structure. The function of the present invention is not substantially constrained by the cross-sectional shape of a gas flux, and the gas supply member can be formed arbitrarily in any shape other than a cylindrical shape on any place other than a plane.
Furthermore, the gas supply member may be made of a conductor, and the gas supply member may be used as the high-potential electrode.
The gas supply member may be made of a dielectric, and the high-potential electrode may be provided in an internal hollow of the gas supply member.
In this case, the high-potential electrode may be provided so as to be integrated with the gas supply member to form a part of an inner surface of the gas supply member, and the medium gas may be in contact with an inner wall surface of the gas supply member and a surface of the high-potential electrode.
Furthermore, the voltage applying element may be capable of supplying a voltage capable of starting partial discharge in the medium gas mass and a voltage capable of maintaining the partial discharge.
Furthermore, the above plasma producing apparatus with the second configuration further includes an auxiliary electrode placed at a position apart from the high-potential electrode so as to be adjacent to a part of the medium gas mass, wherein the auxiliary electrode may be supplied with a ground potential from the voltage applying element.
Furthermore, the above plasma producing apparatus with the second configuration further includes an auxiliary gas supply member that guides the medium gas through an internal hollow, and an auxiliary electrode that is provided in the auxiliary gas supply member and is supplied with a ground potential by the voltage applying element, wherein the auxiliary gas supply member may be placed so that a jet port for jetting the medium gas is in contact with a jet port for jetting the medium gas of the gas supply member or is dose to a jet port for jetting the medium gas of the gas supply member at a predetermined interval g, and at least one of the gas supply member and the auxiliary gas supply member may be made of a dielectric.
Furthermore, the above plasma producing apparatus with the second configuration may be configured so as to produce plasma from a plurality of the medium gas masses and include the high-potential electrode placed in each of the plurality of the medium gas masses.
In the above first method of plasma production, a medium gas stream may be generated as the medium gas mass, and the electric field may be formed by the electric field forming element so that partial discharge occurs from the electric field forming element toward both the upstream side and the downstream side in the medium gas stream.
Furthermore, a strong electric field capable of starting partial discharge in the medium gas mass and a weak electric field capable of maintaining the partial discharge may be formed successively by the electric field forming element.
For forming the electric field by the electric field forming element, a distance between the high-potential electrode and a ground potential portion may be set to be a predetermined distance at which the voltage applied to the high-potential electrode is capable of starting the partial discharge, and a distance between the high-potential electrode and the ground potential portion may be set to be larger than the predetermined distance in a range capable of maintaining the partial discharge.
Hereinafter, the present invention will be described by way of embodiments with reference to the drawings.
A gas supply tube 1 is made of a dielectric, for example, a quartz pipe. A gas tube 2 is connected to a rear end of the gas supply tube 1, and for example, helium (He) gas is supplied to the gas supply tube 1 from a medium gas source (not shown). The helium gas having passed through an internal hollow of the gas supply tube 1 is jetted from a jet port 1a to constitute a gas stream generating portion for forming a gas stream of medium gas. The gas supply tube 1 has an inner diameter of, for example, 50 μm to 50 mm. In place of the quartz pipe, a pipe made of another dielectric, for example, a plastic tube, may be used.
A coaxial single high-potential electrode 3 for producing plasma is set on an outer circumference of an end of the gas supply tube 1 on the jet port 1a side. A voltage applying unit 4 is connected to the high-potential electrode 3 and can apply a positive voltage in a pulse train shape with a predetermined frequency as shown in
Thus, as represented by a broken line in
In order to generate a plasma stream limited in a medium only by partial discharge in the present embodiment, in the above configuration, the gas supply tube 1 and the gas tube 2 function as a gas stream generating portion that generates a medium gas stream, and the high-potential electrode 3 and the voltage applying unit 4 function as an electric field forming portion that forms an electric field corresponding to each medium gas stream. Due to the electric field formed by the electric field forming portion thus provided, partial discharge occurs on both the upstream side and the downstream side in the medium gas stream, and plasma is produced in the medium gas stream from the electric field forming portion toward both the upstream side and the downstream side in the medium gas stream.
In the above configuration, although the voltage applying unit 4 is configured so as to apply a positive voltage in a pulse train shape with a predetermined frequency to the high-potential electrode 3, the applied voltage is not limited to such a form. The applied voltage may have any form as long as it can generate an electric field so as to cause partial discharge.
It is desired to apply a voltage alternating in time. If a voltage alternating in time is applied, plasma is likely to be produced by the alternating component in the voltage, particularly in the case of dielectric barrier discharge, since plasma is ignited via a capacitor of glass. Specifically, a voltage of about 10 kHz may be used; however, a glow-like atmospheric plasma may be obtained even with a voltage at a low frequency of about 60 Hz. When a voltage at a high frequency of about 10 MHz is used, another discharge shape that is uniform even when viewed in any direction by a high-speed camera is obtained. More preferably, a voltage that changes periodically is applied. This is because stable plasma is obtained more easily with periodical discharge.
Although helium gas is preferred as medium gas, another gas also may be used as long as conditions are set appropriately. For example, a mixed gas of argon and ketone also can be used. Furthermore, various processes can be performed by supplying vapor of a chemical entity such as a monomer, or an aerosol such as sprayed mist and fine particles.
The application of the findings about the above discharge mechanism enables various discharges. The LF plasma jet is a thermally non-equilibrium low-temperature plasma, which can be radiated to a base such as thin nylon without causing any damage but has energy sufficient for effecting a surface treatment, ozone generation, and a plasma polymerization.
According to the configuration in which a non-equilibrium plasma jet is generated by a single electrode, i.e., the single high-potential electrode 3 as in the present embodiment, only partial discharge is allowed to occur without causing short-circuit discharge. The number of the high-potential electrode 3, i.e., the electric field forming portion to be placed with respect to one medium gas stream is not limited to one. More specifically, a plurality of electric field forming portions may be provided with respect to one medium gas stream so that each electric field forming portion causes only partial discharge. Thus, in the configuration in which a plurality of high-potential electrodes 3 are placed at a sufficient distance from each other with respect to one gas stream generating portion, the functional effects of the present embodiment also can be obtained.
In the configuration in which only partial discharge is caused to occur, the increase in power consumption involved in short-circuit discharge is suppressed and the energy conversion efficiency can be enhanced, and further, unnecessary heat generation also can be suppressed, compared with a conventional coaxial 2-electrode system. Furthermore, an electrode on a ground side that contributes less to the generation of a plasma jet is omitted, whereby the apparatus is simplified. The production of a plasma jet can be ignited easily even with a single electrode.
Furthermore, according to a method for producing plasma in a space region limited in a medium by a medium gas flux, any medium gas flux is ionized to become plasma stably by causing only partial discharge. The ignition of plasma can be realized on a wide scale of about 10 μm to 50 mm and the increase in an aperture also is possible principally, using the above procedure.
Furthermore, partial discharge is particularly effective for treating the inner surface of a tube. For treating the inner surface of the tube, using a moving electrode (that is not required to be in contact with the tube), a mixture of helium gas and appropriate monomer gas is allowed flow through the tube (only may fill the tube), and plasma is produced inside the tube. This enables the continuous treatment of the tube. If the procedure in the present embodiment is used, the moving electrode can be configured more easily compared with the 2-electrode system.
As described above, in the LF plasma jet producing apparatus in the present embodiment, only a positive voltage in a pulse train shape is applied to the high-potential electrode 3 connected to the gas supply tube 1 through which the medium gas has been allowed to flow, whereby partial discharge is allowed to occur along the medium gas stream dispersed from the gas supply tube 1 to the atmosphere, which can generate a plasma stream. An example of the setting of various conditions for the generation of a plasma stream is as follows.
Medium gas: helium gas
Inner diameter of a quartz pipe: 3 mm
Flow rate of medium gas: several liters/min.
Voltage applied to the high-potential electrode 3: voltage of 10 kV
Frequency of the applied voltage: 10 KHz
Furthermore, even using an electrode (width: 2 mm, length: 50 mm) having no plane dosed in a rotation angle direction with respect to a medium gas flux (electrode covering only a part), plasma can be produced by partial discharge.
The plasma jet according to the present invention has two characteristics: “generation of a gas flux in the atmosphere” and “partial discharge in the vicinity of a high-potential electrode”. Although discharge is allowed to occur by applying a periodical high voltage, plasma parameters can be controlled not only by the applied voltage but also by the applied frequency. The parameters of plasma to be produced can be controlled even by controlling the waveform (polarity) of a high voltage to be applied in addition to the control of the applied voltage and the applied frequency.
The high voltage to be applied actually can be classified into waveforms as shown in
The polarity of the high voltage that is being applied determines the density in the atmosphere, the temperature distribution state, and the like of plasma or ions, electrons, or metastable atoms generated from the plasma. Positive corona discharge occurs in the case of a positive voltage and negative corona discharge occurs in the case of a negative voltage. The positive corona discharge and the negative corona discharge have different physical discharge mechanisms, so that the plasma production state varies. Thus, the use of plasma with each polarity controlled can control the effect of plasma on an object onto which the plasma is radiated. On the other hand, in the case of
By controlling the applied waveforms of positive and negative high voltages in a combination, it can be expected that plasma jets with different parameters are generated and the selective advancement of a chemical reaction is effected.
It is desired that the voltage applying unit 4 is configured so as to change the peak value of an applied voltage at a time of the ignition of plasma and the peak value of an applied voltage at a time of maintaining the production of plasma, as shown in
Furthermore, the high-potential electrode 3 is not required to be provided coaxially on the outer circumferential surface of the gas supply tube 1, and an LF plasma jet can be produced even with an electrode attached to a part of the outer circumferential surface or inner circumferential surface of the gas supply tube 1. More specifically, it is preferred that an electrode is attached to the inner surface or the outer surface of a member made of a dielectric forming a medium gas stream, and the dielectric and the electrode are integrated. When an electrode is attached to the inner surface of a member made of a dielectric, medium gas comes into contact with both the dielectric and the electrode.
Furthermore, the medium gas does not necessarily form a stream. That is, it also is possible to configure a plasma producing apparatus so as to produce plasma from a medium gas mass. In this case, an electric field forming portion that forms an electric field in a medium gas mass is provided. If the medium gas mass has an elongated shape, an electric field is formed so as to cause partial discharge from the electric field forming portion toward both sides in the longitudinal direction of the medium gas mass. The medium gas mass may be configured in such a manner that medium gas is sealed in a tube provided with an electrode. Even in this case, the electrode may be provided on either the inner surface or the outer surface of the tube.
In the present embodiment, the gas supply tube 1 is a quartz pipe made of a dielectric, and a high-potential electrode 6 is a copper wire, which is placed on an axis of an internal hollow at an end of the gas supply tube 1 on the jet port 1a side. If the high-potential electrode 6 is used, the discharge is started from the tip end of the copper wire that is the high-potential electrode 6. Then, a jet extending in an elongated shape increases in a radius gradually toward the jet port 1a of the gas supply tube 1.
As shown in
Furthermore, a coaxial electrode also can be placed on an inner circumferential surface of the end of the gas supply tube 1 on the jet port 1a side in place of the linear high-potential electrode 6. Alternatively, even if an electrode is placed in a part of the inner circumferential surface, a non-equilibrium plasma jet can be produced.
As described above, according to the present invention, a single high-potential electrode may be provided, which increases the degree of freedom of the setting of the electrode. For example, a plasma jet also can be generated using a gas supply tube made of metal as an electrode, in place of attaching an electrode to a gas supply tube made of a dielectric, as in the present embodiment.
In the present embodiment, a gas supply tube is formed of a metal pipe 8 made of a conductive material. The metal pipe 8 is connected to the voltage applying unit 4 and used as a high-potential electrode for producing plasma for applying a positive voltage in a pulse train shape with a predetermined frequency. A plasma jet of a micro size also can be generated, using a metal tube with an inner diameter of about several millimeters, needless to say, or a stainless pipe with an inner diameter of 100 μm as the metal pipe 8.
In the present embodiment, the cross-section of a flat plate-shaped quartz pipe constituting a flat plate-shaped gas supply tube 9 has a flat plate shape instead of the cylindrical shape, as shown in
The LF plasma jet producing apparatus can be enlarged compared with the above embodiments. For example, a non-equilibrium plasma jet 11 in a plane shape of about 2 mm×50 mm can be formed, which is suitable for the treatment of a large area.
Furthermore, as the gas supply tube, a plastic pipe, a metal pipe, or the like can be used in place of the quartz pipe.
The coaxial single high-potential electrode 3 for producing plasma is set on an outer circumference of an end of the gas supply tube 1 on the jet port 1a side. The voltage applying unit 4 is connected to the high-potential electrode 3 and can apply a positive voltage in a pulse train shape with a predetermined frequency. The present embodiment is characterized in that an auxiliary electrode 12 further is placed in the vicinity of the jet port 1a, and is connected to the ground side of the voltage applying unit 4.
If medium gas (for example, helium gas) is jetted from the jet port 1a using the gas supply tube 1 to form a gas stream of the medium gas, and for example, a positive voltage in a pulse train shape of 10 kV is applied with a frequency of about 10 kHz by the voltage applying unit 4, a non-equilibrium plasma jet 5 that extends in an elongated shape from the jet port 1a is generated. At this time, the auxiliary electrode 12 that is grounded is present, which facilitates the ignition of plasma and enhances the stability of maintaining the production of plasma. More specifically, an applied voltage at a time of the ignition of plasma can be reduced to a voltage low enough for maintaining the production of plasma, and the production of plasma can be maintained stably at a sufficiently low voltage.
The auxiliary electrode 12 is placed so as to have such a size as to come into contact with a part of the medium gas stream jetted from the jet port 1a. Thus, the effects of igniting and maintaining plasma can be obtained without having a substantial effect on the generation of the non-equilibrium plasma jet 5.
The present embodiment is characterized in that an auxiliary gas supply tube 13 further is provided adjacent to the jet port 1a of the gas supply tube 1. An auxiliary electrode 14 is placed in the internal hollow of the auxiliary gas supply tube 13, and is connected to the ground side of the voltage applying unit 4. The auxiliary electrode 14 is placed dose to the tube wall of the auxiliary gas supply tube 13 on the gas supply tube 1 side.
The auxiliary gas supply tube 13 is placed diagonally at an acute angle with respect to the gas supply tube 1, and a jet port 13a is placed adjacent to the jet port 1a of the gas supply tube 1. The jet port 13a being placed adjacent to the jet port 1a includes the state in which the they are in contact with each other as shown in
When argon gas, for example, is allowed to flow as medium gas, using the apparatus with the above configuration, and a low-frequency voltage similar to that in Embodiment 1 is applied between the high-potential electrode 3 and the auxiliary electrode 14 by the voltage applying unit 4, the plasma jet 5 can be ignited easily and maintained stably. The reason for this is as follows.
The LF plasma jet is generated by partial discharge instead of short-circuit discharge. The partial discharge is caused by the concentration of an electric field in the vicinity of a high-potential electrode, and therefore, for the production of plasma, a higher voltage is required, compared with that in short-circuit discharge. When helium is used as medium gas, an LF plasma jet can be ignited and maintained at a relatively low voltage. In contrast, argon gas has a higher discharge starting voltage, compared with that of helium gas, so that it is necessary to apply a relatively high voltage. As a result, strong discharge occurs along with the start of discharge. In other words, it is difficult to ignite and maintain an LF plasma jet in argon gas at a low voltage that causes weak discharge which does not impair the features of the LF plasma jet.
In contrast, in the LF plasma jet producing apparatus with the above configuration, the discharge start voltage in the case of using argon gas as medium gas can be decreased by providing the auxiliary gas supply tube 13 having the auxiliary electrode 14. This is ascribed to the fact that the surface creepage 15 first occurs between the high-potential electrode 3 and the auxiliary electrode 14 when a voltage is applied. The surface creepage 15 is a discharge phenomenon along the surface of a solid, and long-distance discharge can be performed at a relatively lower voltage compared with that of the discharge in gas. More specifically, discharge is started at a lower voltage, compared with the partial discharge in a medium gas stream of argon jetted from the gas supply tube 1 by the high-potential electrode 3.
This is because electrons, radicals, UV-rays, or the like are supplied to the periphery by the surface creepage 15, and the discharge start conditions in the peripheral portion become loose. Consequently, even at an applied voltage at which partial discharge is unlikely to occur in a medium gas stream of argon jetted from the gas supply tube 1, the partial discharge by the high-potential electrode 3, i.e., the production of an LF plasma jet is likely to start and the production of plasma can be maintained stably.
The configuration of the present embodiment is effective even when helium gas is used as a medium, because the discharge start voltage is decreased further, and the discharge can be maintained at a lower voltage stably.
As shown in
g/L≦0.1 (1)
Strictly, the value of g/L may be set so that the total of the breakdown voltages in the surface portion and the spatial short-circuit portion is below the applied voltage. However, generally, the spatial breakdown voltage is much higher than the surface breakdown voltage. Therefore, if the total of the breakdown voltages is set in the range represented by Expression (1), practical effects can be obtained.
In the LF plasma jet producing apparatus, surface creepage is allowed to occur along a glass wall by the configuration of a single-sided barrier, in which the high-potential electrode 3 applies a voltage to medium gas, using a glass wall of the gas supply tube 1 as a dielectric barrier, and the auxiliary electrode 14 applies a voltage to medium gas not through the dielectric barrier. On the other hand, surface creepage also can be caused along the glass wall by the configuration of a double-sided barrier, in which the auxiliary electrode 14 also applies a voltage to medium gas, using the glass wall of the auxiliary gas supply tube 13 as a dielectric barrier.
Furthermore, in the above configuration, the auxiliary electrode 14 is placed so as to be biased with respect to a tube axis of the auxiliary gas supply tube 13. However, the auxiliary electrode 14 may be placed at any arrangement, as long as surface creepage is allowed to occur.
A method for producing an LF plasma jet in Embodiment 7 will be described. The LF plasma jet production method in Embodiment 7 is basically similar to that described in Embodiment 1 with reference to
A method obtained by modifying the above basic LF plasma jet production method so as to facilitate the ignition further will be described with reference to front views of
First, as shown in
Then, as shown in
Thus, the applied voltage at a time of the ignition of a plasma jet can be reduced to a voltage lower enough to maintain the production of a plasma jet, which is effective for the miniaturization of the voltage applying unit 4.
A plasma producing apparatus of the present invention is capable of generating a plasma stream stably with a wide range of parameters through a simple discharge mechanism, and is applicable to a wide range of uses including the surface treatment of plastic, the oxidation reaction of a lysate in a solution, and the plasma polymerization of a liquid monomer.
| Number | Date | Country | Kind |
|---|---|---|---|
| 2006-334800 | Dec 2006 | JP | national |
| Filing Document | Filing Date | Country | Kind | 371c Date |
|---|---|---|---|---|
| PCT/JP2007/061837 | 6/12/2007 | WO | 00 | 6/11/2009 |
| Publishing Document | Publishing Date | Country | Kind |
|---|---|---|---|
| WO2008/072390 | 6/19/2008 | WO | A |
| Number | Name | Date | Kind |
|---|---|---|---|
| 5236512 | Rogers et al. | Aug 1993 | A |
| 5316739 | Yoshikawa et al. | May 1994 | A |
| 6652069 | Toda et al. | Nov 2003 | B2 |
| 7576297 | Fujita et al. | Aug 2009 | B2 |
| 20040129220 | Saitoh et al. | Jul 2004 | A1 |
| 20080063576 | Ichiki | Mar 2008 | A1 |
| Number | Date | Country |
|---|---|---|
| 6-065739 | Mar 1994 | JP |
| 2002-313599 | Oct 2002 | JP |
| 2002-368389 | Dec 2002 | JP |
| 2002-368389 | Dec 2002 | JP |
| 2003-282443 | Oct 2003 | JP |
| 2004-111948 | Apr 2004 | JP |
| 2005-267975 | Sep 2005 | JP |
| 2006-060130 | Mar 2006 | JP |
| WO 2006001455 | Jan 2006 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 20100019677 A1 | Jan 2010 | US |
