JP2005264776A - Extra low power plasma reactor system for nox exhaust gas control of automobile - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a plasma reactor and a catalytic converter for reducing NOx of the exhausted matters from an internal combustion engine. <P>SOLUTION: This hyper plasma reactor disposed on a side flow comprises an axial discrete pattern having active and passive electric field areas alternately varying along the axial direction. The hyper plasma reactor develops a high effect on the generation of a plenty of aldehyde when the consumption of an ultra low output and NOx are not present by applying a plasma power to only the gas flow of the side flow including air and hydrocarbon. As compared with the prior art, the less ratio (1 to 2%) of the plasma power is requested. The hyper plasma reactor generates ozone, and the ozone continuously reacts with hydrocarbon to generate the aldehyde (ozone decomposition). The disposition of the side flow of the hyper plasma reactor enables a complete exhaust flow to bypass the side flow without affecting a significant effect on the overall NOx conversion performance of the catalytic converter. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

  The present invention relates to a plasma reactor and a catalytic converter used to reduce NOx in internal combustion engine exhaust, and more particularly to a NOx reduction system based on a plasma reactor and a catalytic converter, the system comprising a catalyst It features a hyper-plasma reactor operating at ultra-low power, located in a side flow position with respect to the main exhaust system to produce abundant amounts of NOx reducing aldehyde upstream of the converter.

The removal of nitrogen oxides (NOx) from internal combustion exhausts is a matter of increasing interest, especially for lean combustion engines such as direct injection gasoline engines and diesel engines. One way to remove NOx after combustion is to subject the exhaust gas to a non-thermal plasma process. At this time, the exhaust gas is passed through the plasma processing apparatus, and a high voltage electric field is involved in the formation of plasma in the apparatus. The plasma has a number of energetic electrons that collide with exhaust gas molecules to form atoms, ions and radicals. These atoms, ions and radicals also react with NO to form NO ₂ or react with hydrocarbons to form aldehydes. The produced aldehyde substantially reduces NOx over a suitable catalyst to form harmless nitrogen. Thus, the primary role of the plasma reactor is to produce NO ₂ from NO and aldehyde from hydrocarbons in the combustion exhaust stream. Of the aldehydes produced in the plasma reactor, acetaldehyde (CH ₃ CHO) is known to be most effective for NO ₂ reduction over alkali-based catalysts.

1A-1C illustrate three prior art plasma reactors, where the external high voltage source is either a pulsating DC power source or an AC power source.
FIG. 1 represents a first form of plasma reactor 10, commonly referred to as a pulsating corona discharge plasma reactor, in which a conductive metal tube 12 forms the wall 14 of the reactor. In the interior, the exhaust gas G passes. Concentric along the axial direction of the tube 12 is a conductive high voltage electrode rod 16. The central electrode rod 16 is electrified by an external high voltage source with the tube 12 functioning as a ground electrode. Here, the corona is formed between them without spark discharge inducing the plasma formation of the exhaust gas.

  FIG. 2 represents a second form of plasma reactor 10 ′, commonly referred to as a dielectric barrier discharge plasma reactor, in which the conductive metal tube 22 and the inner surface of the tube are concentric. Together with the insulating dielectric layer 24 disposed, the reactor wall 26 is formed. As in the first form of plasma reactor 10, the exhaust gas G passes along the inside of the reactor wall 26, and the conductive high voltage electrode rod 28 is concentric with the tube 22 and axially along the center. Has been placed. The central electrode rod 28 is electrified by an external high voltage source with the tube 22 functioning as a ground electrode, and the dielectric layer 24 becomes polarized. The polarization of the dielectric layer 24 accumulates energy, which acts for the purpose of inducing exhaust gas plasma formation without spark discharge.

  FIG. 3 represents a third form of plasma reactor 10 ″, commonly referred to as a dielectric packaged bed discharge plasma reactor, in which the reactor is as in the second form of plasma reactor 10 ′. In addition, a conductive metal tube 32 and an insulating dielectric layer 34 concentrically disposed on the inner surface of the tube together form a reactor wall 36, and exhaust gas G extends along the interior of the reactor wall 36. A conductive high voltage electrode rod 38 passes and is disposed axially along the concentric center of the tube 32. A plurality of small insulating dielectric pellets 40 facilitate exhaust gas G through the space between them. The inside of the reactor wall 36 is filled open so that it can move, and the central electrode rod 38 is electrified by an external high voltage source with the tube 32 functioning as a ground electrode. The dielectric layer 34 is Each of the pellets 40 will also be locally polarized in the same manner, and the polarization of the dielectric layer 34 and the local polarization of the pellets 40 will store energy without the spark discharge. It functions to assist in the induction of exhaust gas plasma formation.

  In the prior art, the plasma reactor walls can have either a flat or cylindrical form. The electrode may typically be made from a continuous electrical connector, where a uniform active electric field is formed in the air gap between them, producing a maximum intensity plasma for a given voltage. To be generated. Prior art plasma reactors enhance the production of high intensity plasmas based on the obvious assumption that plasma intensity is a limiting factor of the underlying process. The continuous electrodes utilized in prior art plasma reactors may be suitable for operating conditions where the supply of high energy electrons is a rate limiting process of the plasma reaction. However, if the rate limiting process is different from the electron supply, increasing the input energy beyond a certain value through a continuous electrode will hardly improve the overall performance of the plasma process.

  While the inventors of the present invention have investigated plasma-assisted lean NOx catalysts, the limiting factor in the plasma reaction process is not the intensity of the plasma, but under typical automotive engine exhaust gas flow operating conditions. It has been discovered that it is a diffusion, mass transport and chemical reaction of intermediate products (eg atoms, ions and radicals) generated in the plasma. Thus, in order to improve the overall performance of the NOx reduction process in engine exhaust, it is important to promote the atomic, ion and radical diffusion, mass transport and chemical reaction processes in the plasma reactor. Become. In this regard, energy is invested in the dielectric layer of prior art plasma reactors without the efficient payment for plasma energy in terms of promoting the maximum reaction of atoms, ions and radicals for NOx and hydrocarbons. The

As shown in FIG. 4, in a typical engine exhaust treatment system 50 using plasma reactor technology, the engine exhaust stream G first passes through the plasma reactor 52 and then the catalytic converter 54. By the way, it passes through the deNOx catalyst. The primary role of the plasma reactor is to convert the NO and hydrocarbons in the exhaust stream to partially oxidized hydrocarbons such as NO ₂ and aldehyde, respectively. In this system, the electrical energy requirement for the plasma reactor is about 20-30 J / L, which results in a power requirement of 600-900 W for an exhaust flow rate of 30 L / s. This prohibitive power requirement for plasma reactors is one of the toughest technical barriers to expand the implementation of this technology in vehicles.

  Therefore, what is needed in the art is somehow to provide abundant amounts of aldehyde upstream of the catalytic converter exhaust by using a plasma reactor operating at ultra-low power.

  During our studies of plasma-assisted lean NOx catalysts using simulated engine exhaust, what has been identified as a rate limiting step in the plasma process under typical operating conditions is various. The mass transport / chemical reaction rate of the kind of ionized reactant (not the electron feed). Ionized reactions by arranging ground electrodes at discrete locations along the axial length of the plasma reactor, thereby providing a passive region between them that serves as an effective mass transport / chemical reaction region It is the inventor's discovery that an increase in mass transport / chemical reaction rate of an object can be achieved.

  In addition, during plasma assisted lean NOx catalyst research, the inventors of the present invention have learned that a key factor in this particular process is the production of aldehydes from hydrocarbons in the plasma reactor. It was known that aldehydes can be produced from hydrocarbons by plasma reactors when NO is present (according to literature reports, aldehyde formation occurs when NO is present in the plasma reactor. Can be ignored). Unlike this well known prior art kinetic mechanism of aldehyde generation in a plasma reactor, the present invention can generate aldehyde from hydrocarbons even when NO is not present in the gas stream passing through, It is a new hyperplasma reactor. This discovery has led the inventor to propose a new reaction mechanism for aldehyde formation in a plasma reactor, namely “ozonolysis for hydrocarbons”. The effectiveness of this new reactor mechanism was confirmed by independent measurements of ozone concentration in the hyperplasma reactor. The unique ability of the hyperplasma reactor according to the present invention to produce acetaldehyde in the absence of NO enabled the inventor to develop a new method for NOx reduction in diesel engine exhaust. According to the present method, the use of a hyperplasma reactor with its own side stream is arranged so that only a small fraction (1% to 2%) of the plasma energy typically required in conventional plasma reactor systems. %) Alone.

  In the hyperplasma reactor according to the present invention, a high voltage (inner) electrode is arranged concentrically with respect to the dielectric plasma wall in the central position along the axial direction, and a ground (outer) electrode has a pattern in which the axial (discrete) electrode is dispersed in the axial direction , Configured to have a spiral pattern or the like that provides an alternating region of active and passive electric fields. The dielectric plasma wall is interfaced at the upstream end to a source of pressurized air, and is interfaced at the other end to a tube connected to the exhaust gas flow. The upstream end is also connected to a hydrocarbon source, such as fuel vapor. This configuration is referred to herein as the “side flow” relationship of the hyperplasma reactor to the exhaust gas flow.

  In operation, the inner electrode is connected to a fluctuating high voltage source, and the outer electrode is connected to ground, thereby providing a continuous active and passive region along the hyperplasma reactor along the axial direction. provide. Incoming air mixed with hydrocarbons experiences a plasma reactor in each active region, followed by a chemical reaction relaxation in the next passive region. In this regard, since each active region is axially compact, intense generation of energetic electrons then occurs. Since each passive region is extended in the axial direction, sufficient time for the resulting oxidation process is provided before encountering the next active region. Thus, the energy consumption associated with aldehyde formation is very favorable.

  This favorable result is explained as follows. Since the velocity of ions and radicals depends on the strength of the electric field, these velocities in the radial direction (direction intersecting the axial direction) are faster in the active region than in the passive region. This radial velocity gradient is aided by the spatially alternating electric field to promote axial mixing of the intermediate product of the ionization reaction and consequently improve reactivity with the hydrocarbon. This mixing is then performed in order for the hyperplasma reactor according to the present invention to require much less energy to operate and to achieve the same level of performance as the prior art plasma reactor. It means that it can be compact.

  The NOx reduction system of the hyperplasma reactor according to the present invention is very effective in terms of ultra-low power consumption and abundant production of aldehyde when NO is not present. The present invention eliminates unnecessary power consumption applied to a complete exhaust gas stream by applying plasma power only to a side stream gas stream containing air and hydrocarbons to produce aldehydes. Thus, only a small fraction (1% to 2%) of the plasma power is required compared to the power for the prior art plasma reactor to process the complete exhaust gas stream. The hyperplasma reactor produces ozone, which reacts continuously with hydrocarbons to produce aldehydes (ozonolysis). The side flow arrangement of the hyperplasma reactor allows the complete exhaust flow to bypass the side flow without significantly affecting the overall NOx conversion performance in the catalytic converter. Furthermore, the side flow arrangement of the hyperplasma reactor allows the hyperplasma reactor to operate at conditions independent of the catalytic (de-NOx catalyst) converter and the main exhaust stream.

  Objects, features and advantages of the present invention will become more apparent from the following description of preferred embodiments.

  Referring now to the drawings, FIGS. 5 to 16 illustrate various aspects of an example of an automobile exhaust gas hyperplasma reactor and catalytic converter system 1000 according to the present invention. Here, the hyperplasma 100 of the present invention is characterized by a continuous alternating region of active and passive electric fields along its axial length. The hyperplasma reactor is arranged in a side flow relationship with respect to the main exhaust flow, as shown in FIG.

  As shown in FIGS. 6 to 9, the hyperplasma reactor 100 according to the present invention functions as a dielectric barrier, and a plasma reaction formed of an insulating dielectric material 102 ′ that forms the space of the reactor therein. It has an elongated cylindrical shape formed by the vessel wall 102. The configuration of the plasma reactor wall 102 may be any suitable dielectric material such as quartz, glass, alumina, and the like. By way of example only and not limitation, the dielectric material may be a quartz tube having an outer diameter of 9.5 mm (3/8 inch) and a wall thickness of 1 mm. The inlet 106 is disposed at one stage of the plasma reactor wall 102 and the outlet 108 is disposed at the other end of the plasma reactor wall. A protective metal shell 122 covers the hyperplasma reactor 100 (shown broken for clarity).

  The high voltage conductive center (inner) electrode rod 110 is located at the concentric center of the plasma reactor wall 102. The central electrode rod 110 extends in common with the plasma wall and is fixed to the wall. The center electrode rod 110 can be formed of any conductive material, such as stainless steel, aluminum, copper, and the like. By way of example only and not limitation, the center electrode rod 110 may be constructed from stainless steel having a diameter of 3.2 mm (1/8 inch). The center electrode rod 110 is connected to the high voltage output of a time varying high voltage source 112 (see FIG. 8). For example, a dielectric material may cover the central electrode rod for the purpose of electrode protection from a corrosive exhaust gas environment.

  A conductive ground (outer) electrode 114 is wound tightly (in contact) with a selected pitch, providing a discrete spacing d in the axial direction, around the plasma reactor wall 102, a wire 114 ′ ( The term “wire” is meant to include all its equivalents, such as a narrow thin conductive film.) In this regard, the ground electrode is a series of discretely spaced. Arranged in a continuous pattern including positions, the continuous pattern being arranged with respect to axis F, along which the air mixed with hydrocarbons flows (see below). The pitch is provided to provide, for example, a coarse interval (preferred example), a tight interval, a constant interval (preferred example), or a variable interval. The ground electrode 114 is connected to the ground of the high voltage source 112. By way of example only and not by way of limitation, the ground electrode 114 may be composed of a small gauge copper / nickel wire coiled tightly around the plasma reactor wall 102.

  The outer surface region of the plasma reactor wall 102 that is in local contact with the ground electrode 114 (the wire 114 ′ thereof) is the active of the electric field formed by the galvanic interaction between the electrode rod 110 and the ground electrode. Region 116 is formed, and the electric field is adjusted by the polarization of the dielectric material of plasma reactor wall 102. The space between the active regions 116 along the axial direction in the plasma reactor wall 102 constitutes a passive region 118 of the electric field. The active region 116 of the electric field has a higher field strength than the passive region 118. The resulting axially changing electric field is represented by plot 120 in FIG.

  In FIG. 9, the axial position 120a of the active region of the ground electrode and the accompanying electric field strength is indicated by a rectangular solid line bar. The non-uniform electric field strength 120b is indicated by a broken line. The smooth transition of the inhomogeneous electric field strength between the active region 116 and the passive region 118 is due to the free drift of high energy electrons from the active region to the passive region. This drift comes from the physical nature of the free boundary between the active and passive regions.

  It has been determined that the optimization of the active and passive regions of the electric field of the plasma reactor 100 according to the present invention can be expressed by the following relational expression.

Here, d (eg, shown in FIG. 6) is the distance between the active and passive regions that are connected to each other (ie, the axial length of the passive region) and h (eg, in FIG. 7). Is the shortest distance between the center electrode rod and the outer ground electrode. The exact value of d depends on the specific kinetics of the chemical reaction occurring in the plasma reactor.

  Experiments demonstrating the success of the plasma reactor 100 were performed using a simulated engine exhaust gas mixture. What was observed was an annular region with high brightness between the central electrode rod and the (quartz tube) dielectric plasma reactor wall. The brightness of the area represented the presence of exhaust gas plasma. On the outer surface of the plasma reactor wall, what was observed was a high intensity region adjacent to the outer ground electrode spiral wire, which represented the active region of the electric field. What was further observed on the outer surface of the plasma reactor wall was a dark area between the high intensity areas. The region represented the passive region of the electric field. Despite this apparent difference between the active and passive regions of the electric field, as shown on the outer surface (dielectric barrier) of the plasma reactor wall, the plasma intensity in the annular region can be almost uniform. Observed and suggests the presence of a good gas phase mixing in the plasma. This result can be explained as follows. Since the ion velocity depends on the strength of the electric field, it is faster in the active region of the electric field than in the passive region of the electric field. This facilitates the axial mixing of the intermediate product of the ionization reaction when using an alternating electric field, resulting in improved reactivity of NOx.

  Referring now to FIG. 5, it can be seen that the aforementioned hyperplasma reactor 100 is located at a side flow position with respect to the main exhaust flow G at a position upstream of the catalytic converter 124. The catalytic converter 124 is suitable for executing a deNOx catalyst when, for example, a NaY catalyst is used.

Entering the inlet 106 is air Ar emanating from any suitable pressurized air source 126, which may be, for example, a brauer. Also entering the inlet 106 is a stream of hydrocarbon molecules HC originating from any suitable source 128. This source may be, for example, a tube connecting to a fuel vapor source or a connection connecting a small amount of engine exhaust gas upstream of the catalytic converter to the tap. This hydrocarbon-supporting air A _R + HC passes through the hyperplasma reactor 100.

In operation, the inner electrode 110 is connected to a variable high voltage source 112 and the outer electrode 114 is connected to ground, thereby continuously active along the hyperplasma reactor in the direction of A _R + HC flow axis F. Region 116 and passive region 118 are provided. Incoming air mixed with hydrocarbons experiences a plasma reaction in each active region, followed by chemical reaction relaxation in the next passive region. In this regard, since each active region is axially compact, intense generation of energetic electrons then occurs. Since each passive region is extended in the axial direction, sufficient time for the resulting oxidation process is provided before encountering the next active region. As a result, abundant aldehydes are produced. The energy consumption associated with the production of aldehydes is very favorable. This aldehyde loaded with air A _R + A passes to the catalytic converter 124 where the aldehyde provides a reaction for the NOx reduction catalyst.

  Referring now to FIGS. 11-16, various test results for the operating characteristics of the hyperplasma reactor 100 in combination with the catalytic converter 124 are shown. In this regard, FIGS. 10A and 10B represent a diesel engine dynamometer facility for these test results.

  FIG. 10A is a schematic flow diagram of a diesel engine dynamometer test facility 130 in which a conventional plasma reactor 56 and a de-NOx catalytic catalytic converter 58 are exhausted for performance testing under diesel engine exhaust conditions. Installed due to side flow. Detailed test conditions are listed in Table II.

Table II
Engine (1.3L, 3 cycle Isuzu) :
Speed = 2300rpm
Torque = 25Nm
BMEP = 250kPa
EGR = 0-45%
Fuel = FT
Exhaust gas temperature: 217C
Exhaust gas composition:
HC = 21 ppm (C ₃ )
NOx = 265ppm
O ₂ = 15%
CO ₂ = 3.8%
CO = 142ppm
Conventional plasma reactor:
Cylindrical shape
SV = 60K / h
Ep = 30J / L
T = 150C
Catalytic converter:
Catalyst = NaY, Ba / NaY
Reactor = 5.1 cm (2 inch) diameter pipe, packed bed
SV = 10-30K / h
T = 200C
Side flow:
Flow rate = 10-30L / min
Reducing agent injection = FT fuel, 2-butene FIG. 10B used the same Table I except that a small cylindrical hyperplasma reactor 100 ′ according to the present invention was installed in the second side flow. FIG. 3 is a schematic flowchart of a dynamometer test facility 130 ′ for a diesel engine. A hydrocarbon HC reducing agent (2-butene) is injected into the second side stream, and air is introduced. Both are injected before the hyperplasma reactor. Note that the hyperplasma reactor 100 "in this second side stream is used as a hydrocarbon reformer to produce aldehyde from hydrocarbons independently of the engine exhaust stream. The effluent was supplied to the main sidestream exhaust before the catalytic converter 124 'of the NOx removal catalyst.

  FIG. 11 shows the production of aldehyde from propylene by the hyperplasma reactor according to the present invention with and without NO present in the feed stream. The feed stream maintained a simulated exhaust gas composition containing 600 ppm propylene, 12% oxygen, 2.5% water vapor, 225 ppm (or 0 ppm for comparison) NO, and balance nitrogen. FIG. 11 clearly demonstrates that the hyperplasma reactor according to the present invention can actually produce an aldehyde in the absence of NO. This finding is in contrast to the well established literature reports that prior art plasma reactors cannot produce significant amounts of aldehydes without NO in the feed stream.

FIG. 12 shows the ozone concentration in the hyperplasma reactor according to the present invention. The feed stream maintained a simulated exhaust gas composition comprising 600 ppm propylene, 12% oxygen, 2.5% water vapor, 225 ppm (or 0 ppm for comparison) NO, and balance nitrogen. The hyperplasma reactor had an energy density of 20 J / L with SV = 25 K / h and O ₃ maintained about 30 ppm. Most of the ozone produced was consumed by propylene and the rest was consumed by NO. It is noteworthy that under full flow conditions there remains a substantial amount of ozone that can still be useful in the hyperplasma reactor. This high concentration of ozone is an important means that makes it possible to produce aldehydes via “hydrocarbon ozonolysis”.

  FIG. 13 compares aldehyde formation with propylene and 2-butene. The feed stream was simulated including 600 ppm propylene (or 450 ppm 2-butene), 12% oxygen, 2.5% water vapor, 225 ppm (or 0 ppm for comparison), and balance nitrogen. The exhaust gas composition was maintained. The hyperplasma reactor had SV = 25 K / h and an energy density of 20 J / L. 2-Butene produces more acetaldehyde (+ 70%) and less formaldehyde (-60%) compared to propylene according to the ozonolysis mechanism.

  FIG. 14 shows the NOx conversion performance of the plasma / catalyst system with 2-butene injected as a reducing agent in a diesel engine dynamometer experiment. The NOx conversion initially reached 93%, but slowly decreased to a steady state value of 87% within 5 hours.

FIG. 15 compares the efficiency of 2-butene and Fischer-Tropsch (FT) diesel fuel injected as a reducing agent. The deNOx catalyst used in this case was Ba / NaY. As shown in FIG. 15, 2-butene is an FT diesel fuel for both NO conversion to NO ₂ in the plasma reactor and overall NOx conversion across the combined plasma / catalyst system. Better.

  FIG. 16 illustrates the performance of a conventional plasma reactor 56 when the hyperplasma according to the present invention is used with a deNOx catalyst (NaY in this case) as schematically illustrated in FIGS. 10A and 10B, respectively. Comparison is made in terms of the performance of the reactor 100 ′, NOx conversion rate, and plasma energy consumption. Hyperplasma reactors used as side stream hydrocarbon reformers are very low in operation when compared to prior art plasma reactors used in the main side stream to treat engine exhaust It's worth noting that power is enough. The slight decrease in NOx conversion (87% to 77%) for the hyperplasma reactor system (FIG. 10B) compared to the conventional plasma reactor system (FIG. 10A) is negligible. It is believed that the present invention can correct this minor undesirable effect by optimizing the design parameters of the hyperplasma reactor.

In summary, the test results show that:
1. Hyperplasma reactors (or superactive plasma reactors) provide excellent activation for partial oxidation of hydrocarbons. In particular, the novel plasma reactor can produce aldehydes from hydrocarbons even in the absence of NO in the gas stream.
2. The hyperplasma reactor can generate a non-uniform electric field axially in the direction of air movement through the reactor. The strength of the electric field can be easily adjusted to best fit different hydrocarbon types.
3. Hyperplasma reactors can generate large amounts of ozone from engine exhaust gas composition by using very low plasma power.
4). NaY catalyst has been identified as the best catalyst for the hyperplasma reactor and catalytic converter system according to the present invention for NOx reduction in diesel engine exhaust.
5). Among the hydrocarbons, 2-butene has been identified as the best reducing agent for the hyperplasma reactor and catalytic converter system according to the present invention for Ox reduction in diesel engine exhaust.
6). A new method of aldehyde production has been found that uses a hyperplasma reactor (or plasma reforming) in a side stream independent of engine exhaust. This plasma reforming in the side stream allows the hyperplasma reactor to be selectively controlled independent of the deNOx catalyst and engine exhaust flow.
7). The new method of aldehyde production according to the present invention allows ultra-low levels (e.g. 600 to 900 W in the case of the conventional system compared to 10 to 15 W, i.e. Allows to operate the hyperplasma reactor.

  For those skilled in the art to which the present invention pertains, the preferred embodiments described above can be subject to change or modification. For example, the plasma reactor wall can have any suitable shape. Such changes or modifications are limited only by the scope of the appended claims and can be made without departing from the scope of the invention.

FIG. 1 is a partial cross-sectional side view of a prior art plasma reactor. FIG. 2 is a partial cross-sectional side view of a prior art plasma reactor. FIG. 3 is a partial cross-sectional side view of a prior art plasma reactor. FIG. 4 is a schematic diagram of a prior art plasma reactor and catalytic converter in an exhaust gas NOx removal system. FIG. 5 is a schematic view of a hyperplasma reactor and a catalytic converter in the exhaust gas NOx removal system according to the present invention. 6 is a partial cross-sectional side view of the hyperplasma reactor of FIG. FIG. 7 is a cross-sectional end view taken along line 7-7 of FIG. FIG. 8 is a schematic diagram of an electrical circuit for the hyperplasma reactor of FIG. FIG. 9 is a plot on the graph of electric field strength versus axial distance in the hyperplasma reactor of FIG. FIG. 10A is a schematic diagram of a dynamometer test facility. FIG. 10B is a schematic diagram of a dynamometer test facility. FIG. 11 is a plot illustrating various operating characteristics of the hyperplasma reactor and the hyperplasma reactor / catalytic converter system of FIG. FIG. 12 is a plot illustrating various operating characteristics of the hyperplasma reactor and the hyperplasma reactor / catalytic converter system of FIG. 13 is a plot illustrating various operating characteristics of the hyperplasma reactor and the hyperplasma reactor / catalytic converter system of FIG. 14 is a plot illustrating various operating characteristics of the hyperplasma reactor and the hyperplasma reactor / catalytic converter system of FIG. FIG. 15 is a plot illustrating various operating characteristics of the hyperplasma reactor and the hyperplasma reactor / catalytic converter system of FIG. 16 is a plot illustrating various operating characteristics of the hyperplasma reactor and the hyperplasma reactor / catalytic converter system of FIG.

Claims (14)

An exhaust gas treatment system for an internal combustion engine comprising:
Exhaust gas flow piping;
A hyperplasma reactor having an inlet and an outlet on the opposite side, the dielectric plasma reactor wall forming the reactor space, and being disposed in the reactor space parallel to the dielectric plasma reactor wall An inner electrode and an exit electrode adjacent to the dielectric plasma reactor wall, the exit electrode being arranged in a series of discretely spaced continuous patterns, the continuous patterns being arranged relative to an axis The exit electrode, and the hyperplasma reactor,
A first source connected to the inlet to provide air;
A second source connected to the inlet to provide hydrocarbons;
A catalytic converter connected to the pipe;
A connection formed between the outlet and the pipe at an upstream position with respect to the catalytic converter;
With
An exhaust gas treatment system, wherein air from the first source mixes with hydrocarbons from the second source, the mixture flows into the inlet, passes through the reactor space, and exits from the outlet. The exhaust gas treatment system according to claim 1, wherein the outer electrode is composed of a conductive wire and an equivalent thereof, and the inner electrode extends substantially at the center together with the dielectric plasma reactor wall. The exhaust gas treatment system according to claim 2, wherein the dielectric plasma reactor wall has a cylindrical shape, and the wire is spirally wound around the dielectric plasma reactor wall with respect to the axis. Further comprising a time-varying high voltage source connected to the inner and outer electrodes, the voltage source being parallel to the axis relative to the inner and outer electrodes and the dielectric plasma reactor wall. The exhaust gas treatment system of claim 1, wherein the region provides a continuously alternating region of active and passive electric fields in a direction along the dielectric plasma reactor wall. Each of the active regions of the electric field has an active distance parallel to the axis that is shorter than a passive distance parallel to the axis of any passive region of the electric field, wherein the passive distance is substantially Defined by

5. The exhaust according to claim 4, wherein d is a length parallel to the axis of the passive region of the electric field, and h is a shortest distance between the inner electrode rod and the outer electrode. Gas processing system. The exhaust gas treatment system of claim 5, wherein the continuously alternating regions of the active and passive electric fields provide an effective capacitance of the plasma reactor that exceeds a capacitance inherent in the plasma reactor. The exhaust gas treatment system according to claim 6, wherein the outer electrode is composed of a conductive wire and an equivalent thereof, and the inner electrode extends approximately at the center together with the dielectric plasma reactor wall. The exhaust gas treatment system according to claim 7, wherein the dielectric plasma reactor wall has a cylindrical shape, and the wire is spirally wound around the dielectric plasma reactor wall with respect to the axis. A method for providing an aldehyde comprising:
Provide air flow along the axis,
Mixing hydrocarbons into the air stream to provide a hydrocarbon mixed air stream;
Subjecting the hydrocarbon-mixed air stream to a high voltage region extending over a short distance parallel to the axis;
Immediately thereafter, subjecting the hydrocarbon mixture air stream to a voltage lower than the high voltage over a long distance parallel to the axis;
The first and second voltage exposure steps are continuously repeated a selected number of times, each step comprising a hydrocarbon ozonolysis process substantially during the first voltage exposure step during the carbonization step. A method wherein the aldehyde is generated in a hydrogen mixed air stream and the aldehyde is produced by the ozonolysis process of hydrocarbons during the first and second voltage exposure steps. The method of claim 9, wherein energy is substantially supplied only during each of the first voltage exposure steps for ozonolysis of hydrocarbons. The method of claim 10, wherein the hydrocarbon-mixed air stream is substantially free of NO. A method for treating exhaust gas of an internal combustion engine, comprising:
Provide air flow along the axis,
Mixing hydrocarbons into the air stream to provide a hydrocarbon mixed air stream;
Subjecting the hydrocarbon-mixed air stream to a high voltage region extending over a short distance parallel to the axis;
Immediately thereafter, subjecting the hydrocarbon mixture air stream to a voltage lower than the high voltage over a long distance parallel to the axis;
The first and second voltage exposure steps are continuously repeated a selected number of times to provide an aldehyde-mixed air stream, whereby the hydrocarbon ozonolysis process substantially comprises the first An aldehyde is produced by the ozonolysis process of hydrocarbons during the first and second voltage exposure steps;
Mixing the aldehyde mixed air stream with an internal combustion engine exhaust gas stream to provide an aldehyde mixed exhaust gas stream;
A method comprising treating each exhaust gas stream mixed with the aldehyde with a catalyst. The method of claim 12, wherein energy is substantially supplied only during each of the first voltage exposure steps for ozonolysis of hydrocarbons. 14. The method of claim 13, wherein the hydrocarbon-mixed air stream is substantially free of NO.

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