Patent Grant
6902604
The invention relates to electrostatic precipitators, including for diesel engine electrostatic crankcase ventilation systems for blowby gas for removing suspended particulate matter including oil droplets from the blowby gas.
Electrostatic precipitators, including for diesel engine electrostatic crankcase ventilation systems, are known in the prior art. In its simplest form, a high voltage corona discharge electrode is placed in the center of a grounded tube or canister providing an annular ground plane around the electrode. A high DC voltage, such as several thousand volts, e.g. 15 kV, on the center discharge electrode causes a corona discharge to develop between the discharge electrode and the interior surface of the tube providing a collector electrode. As the gas containing suspended particles flows between the discharge electrode and the collector electrode provided by the wall of the tube, the particles are electrically charged by the corona ions. The charged particles are then precipitated electrostatically by the electric field onto the interior surface of the collecting tube.
Electrostatic precipitators have been used in diesel engine crankcase ventilation systems for removing suspended particulate matter including oil droplets from the blowby gas, for example so that the blowby gas can be returned to the fresh air intake side of the diesel engine for further combustion, thus providing a blowby gas recirculation system.
In known electrostatic precipitators, the high voltage power supply is placed outside the collector section, either remotely mounted or mounted directly to the collector in some manner. In either of these configurations, a high voltage electrode rod or lead must pass-through an insulator section to deliver the high voltage to the corona producing discharge electrode assembly. The insulator may also be heated to prevent moisture and contaminant accumulation on the insulating surface, thereby reducing the insulating properties of such section.
The present invention eliminates the need for the noted high voltage pass-through of a high voltage lead through the noted insulator. In the present invention, the high voltage power supply is disposed internally of such insulator, and in the preferred embodiment is in the hollow interior of the corona discharge electrode assembly. This eliminates the need for any external high voltage cables or connections and eliminates the need for the high voltage pass-through of a high voltage lead through the insulator.
The present invention relates to improvements arising during continuing development efforts related to the subject matter of U.S. Pat. No. 6,221,136, incorporated herein by reference. The drawings and specification of the '136 patent are set forth below.
An electric heater 22 is in contact with the insulator bushing 18 to keep the insulator bushing at a sufficiently high temperature to prevent vapor condensation and particle deposition on the bushing 18.
Gas containing suspended droplets and other particulate matter from a source 23 is directed to flow through an inlet opening 24 of the housing 12 and passes through a porous medium 26 in the inlet. The porous medium 26 is a relatively inefficient droplet collector to keep out large contaminants, so that most of the droplets in the aerosol are carried by the gas into the electrostatic electrode region or chamber 28 above.
The input gas then flows around the electrode assembly 14 to expose the droplet particles in the gas to the high electric field around the electrode assembly. The discharge electrode assembly 14 includes a central rigid support 30 for two support discs 32 and 34 on opposite ends of the central support. The upper disc 32 may be attached to the insulator bushing 18 and thus support the discs 32 and 24 from the housing 12. A plurality of holes 35 (see
The gas (aerosol) flows around the wires 36 and ions are produced in the corona discharge. The ions collide with the droplets to cause the droplets to be charged. The charged droplets are then carried by the gas flow through an electrically conducting, grounded porous medium 40 as the gas flows to an outlet 42. The droplets are collected by electrostatic precipitation onto the grounded collecting elements in-the medium.
The clean gas then flows out of the annular space 41 between the porous medium 40 and the outer housing 12 to the outlet 42. The collected oil droplets flow down the inside surface of the porous medium 40 as a thin film which is returned by gravity to an oil reservoir or sump 44.
As shown in
Using a thin wire of a uniform diameter in the above electrode arrangement, and in other embodiments disclosed, it is important to keep the distance between each wire segment and the adjacent collector electrode the same for all the wire segments on the support structure. By keeping the distance uniform and using the same high voltage potential on all the wire segments, a uniform corona discharge can be maintained. This will insure that all particles flowing through the device will be charged uniformly and to the same maximum possible extent to insure high collection efficiency for the device.
In designing an electrostatic precipitator using the above electrode assembly, the spacing, S, between the wire segments must bear a proper relationship to the distance, D, between the wire segment and the adjacent collector electrode surface. (see FIG. 2). Too small a spacing, S, will cause the closely spaced wire segments to interfere with each other, thereby reducing the maximum current that can be obtained from each wire. Too large a spacing will cause some empty spots on the collector electrode surface to appear. Within these empty spots, there are no corona current flow. Particles flowing over these empty spots will not encounter corona ions and thus remain uncharged. From experience, it has been found that the ratio, S/D, must be kept between the limits of 0.1 and 10, preferably between 0.3 and 3, for the electrode assembly to function properly and avoid degradation in performance.
For application in a Diesel blowby gas recirculation system, the inlet housing 24 is connected to an opening in the crankcase, which is represented at 23, and the collected oil film is also returned directly to the crankcase. The outlet 42 can be open to the atmosphere to allow the cleaned blowby gas to be discharged to the atmosphere, or the outlet 42 can be connected to the intake of the Diesel engine for exhaust gas recirculation.
The total discharge electrode length is greatly increased from that of the conventional precipitator with a single discharge electrode in the center of a tube. The corona current that can be maintained between the discharge electrode and the collecting tube is generally proportional to the total electrode length. The approach described here makes it possible to greatly increase the electrode length and hence the total corona current, thereby increasing the efficiency for both droplet particle charging and precipitation of the charged droplets or particles. A laboratory prototype device has demonstrated the practicality of this approach. As many as sixteen discharge electrodes have been used leading to approximately a factor of sixteen increase in total corona current in laboratory prototypes.
Another purpose of the electrode design shown is to allow the discharge electrode to be circumferentially supported on a circle. A large diameter circle of the electrode length mounting will bring the discharge electrodes (the wires) closer to the porous medium 40 collecting surface, thereby reducing the voltage needed to maintain the corona discharge between the electrode and the grounded porous collecting surface. A lower operating voltage from existing precipitators is desirable for the applications described above, to reduce the need for very high voltage insulation. When using a lower voltage, the leakage current through the insulator bushing 18 can be reduced. Using a lower voltage also reduces the cost and complexity of the power supply 16, thus making the device more economical to produce. In the present device, voltages of between 5,000 to 10,000 volts are most preferred, but voltages up to 20,000, volts DC can be used.
Using a circle of electrode lengths spaced from the center rod also forces the gas flowing radially outward toward the porous collecting surface to be exposed to the very high electric field surrounding each discharge electrode. Generally, the electric field strength according to Gauss's law tends to decrease with increasing distance from the discharge electrode. The closely spaced wires forming the discharge electrodes forces the gas to pass through the high field region between the electrodes and to be exposed to the high electric field around the wires. Each droplet or particle can thus be charged to a higher level than is possible with the conventional single length electrode design, thereby gaining a higher electrical charge and allowing droplets to be more easily removed by electrostatic precipitation.
Although a porous collector electrode 40 is shown in
The high-voltage insulator bushing 18, if unprotected, will be exposed to the suspended droplets or particles in the gas, as well as any condensable vapor which may be present. Over time, the accumulation of deposited and condensed material on the insulator will render it ineffective. The insulator is heated by contact with the electrical heating element 22 to a high enough temperature to prevent vapor condensation on the insulator bushing.
To prevent the precipitation of droplets or particles on the insulator bushing surface, a conductive shroud or shield 20 surrounds the insulator. This conductive shroud 20 is connected to the same high voltage source as the discharge electrodes 36 so that a high electric field is created in the region between the shroud and the nearby grounded surfaces of the porous medium 40 or housing 12. The charged droplets or particles present in the gas will thus be precipitated onto the grounded surfaces and not on the high voltage insulation bushing.
Design variations of conductive shroud 20 are shown in
In
In
The top wall 64 of the housing is spaced from the plate 60, to form a gap 66 between the housing wall 64, which is a top wall, and the plate 60 which is a shielding disc. The support 68 can be used for supporting a top plate 32 of the electrode assembly as before.
Each of these forms of conductive shroud shows a gap between the high voltage shield or shroud and a portion of the grounded housing. The gap is relatively narrow, and will provide for precipitation of charged particles that come near the high voltage shield, to the walls of the grounded housing.
Creating a long pathway in the gap space as shown in
In spite of the efficient high voltage insulator shield design of this invention, there is the possibility that some droplets or particles in the gas may remain uncharged. These uncharged particles will be capable of penetrating through the gap space 56 or 66 between the shroud and the nearby grounded surface to deposit on the insulator. The precipitation of these uncharged particles on the insulator can be prevented by utilizing the phenomena of thermophoresis. Thermophoresis refers to the movement of aerosol particles in the direction of a decreasing temperature gradient due to the radiometric force acting on the particles. For effective thermophoretic motion of the particles to prevent particle precipitation on the insulator the insulator must he held at a sufficiently high temperature. The insulator temperature must be 10° C. or more than the surrounding gas temperature. In contrast, to prevent vapor condensation, the insulator only needs to be held above the dew point of the condensable species in the gas. Usually at least a few degree C above the gas temperature would be sufficient
To be effective, the porous medium 40 must be made of a conductive material, usually metal. It can be made of a perforated metal, a porous, sintered metal, one or more layers of wire mesh material rolled into the desired cylindrical shape, a pad of metal fiber or wires formed into a cylinder, and similar configurations. As the gas flows into the porous medium, particles are brought to close proximity to the surface of the conducting elements in the medium, thus allowing the charged particles to be effectively deposited onto the surface of the conducting elements of the porous medium. In comparison, in the conventional electrostatic precipitator using solid collecting electrodes, such as a solid tube surrounding the center electrodes, the charged particles must be precipitated by electrical force through the fluid boundary layer adjacent to the inner surface of the surrounding tube.
Depending on the gas flow velocity, the relatively stagnant boundary layers adjacent to the solid collecting surfaces may be a centimeter or more in thickness. The particles must be precipitated through this centimeter thick stagnant gas layer to be deposited on the surface. In comparison, using a porous collecting electrode, as shown here, the gas is forced to flow between the closely spaced conducting elements in the porous medium, thereby greatly reducing the distance the particles must travel to reach the collecting surface. This will increase the efficiency of the precipitator and reduce the overall physical size of the device.
Not all electrically conducting porous material can be used with the compact electrostatic precipitator described in this invention. In order to handle the high gas flow rate per unit of collecting surface intended for this application, the porous material must not produce excessive pressure drop at the required high gas flow. In addition, the collected oil drops must drained off easily by gravity and not be collected in the porous medium to clog the medium or produce excessive high pressure drops. Depending on the structure of the porous medium, and the surface tension and viscosity of the liquid droplets being collected, the distance between the conducting elements of the porous medium must be kept above a critical limit. Too small a distance will allow the collected droplets to form surface films bridging neighboring elements and block the flow. For the usual liquid such as lubricating oils, the mean distance between the conductive elements in the medium must be larger than about 5 microns, and preferably larger than 10 μm. The mean distance between the elements in a porous medium is also referred to as the mean pore diameter which can be measured by a commercial poremeter. A mean pore diameter greater than 5 μm, preferably greater than 10 μm, is generally necessary for the medium to work successfully as the porous collecting electrode of the droplet collecting precipitator described herein.
There are a number of devices using a porous medium to collect charged particles. One such device is the electrically augmented bag filter described by Penney in U.S. Pat. No. 3,910,779. In Penney's device, the particles are charged in a corona charger. The charged particles are then carried by the gas flow through a fabric medium and deposited on the surface of the fabric. The particles to be deposited must be a dry solid material, so that the deposited particles on the fabric will form a porous cake. Since a cake will also form on the fabric in the absence of an electrical charge, electrostatics charges are used by Penney to modify the property of this cake namely to increase the pore size of the cake and reduce the pressure drop. The textile fabric used in a fabric filter is usually not electrically conductive, so that it is not possible to maintain a corona discharge directly between the corona electrode and the fabric. A separate corona charger is used upstream of the fabric filter to charge the particles for subsequent filtration by the fabric.
Another device using a porous filter media is what is usually referred to as electrostatically enhanced fibrous filter such as that described by Carr in U.S. Pat. No. 3,999,964. A conventional fibrous filter media made of glass, polymeric and other non-conducting fibers is sandwiched between two sets of electrical grids. A potential difference is established between the grids to create an electric field in the medium to enhance the efficiency of the medium for particle collection by electrostatic attraction. The device is most effective when the particles are electrically charged. If the particles are not charged, a corona ionizer can be used upstream of the filter to charge the particles to increase the efficiency of the filter for particle collection.
A further version of the electrostatically enhanced fibrous filter is that of Argo et al in U.S. Pat. No. 4,222,748. In Argo's device, a corona charger is used upstream to charge the particles. As the charged particles are collected in the fiber bed, which is made of a non-conductive material, charge will build up in the bed to raise its electrical potential. To prevent the continuous buildup of charge in the bed, the bed is continuously irrigated by water to make the bed conductive. Particles collected in the bed are also carried away by the flowing water.
The electrostatic precipitator of the '136 patent is very efficient and can be made into a small compact size. For many applications, such as diesel blowby filtration, the cylindrical geometry with a circular cross section is the most convenient. However, it is not necessary that the cross section shape be a circle to take advantage of many of the features of this invention. Rectangular, elliptical, and other cross sectional shapes can be easily adapted to the design of an electrostatic precipitator described by the method described in the present invention.
In designing such a rectangular precipitator, it is important to keep the individual corona wire lengths between the support 74 at approximately the same distance from the porous collecting electrode 78. This will insure that the corona discharge between the high voltage corona wire 76 and the collecting electrode 78 will be uniform at the same applied voltage on the wires. As before, the lateral distance between the wire lengths and the porous collecting electrode 78 can be reduced to lower the required operating voltage of the precipitator.
Although the precipitator described in the '136 invention is intended for droplet aerosol collection, it can also be used to collect aerosols containing only dry solid particles. To prevent the build up of solid particles in the porous collecting electrode which will cause plugging of the pores, liquid droplets, usually water, can be added to the aerosol before it is introduced into the precipitator.
Because of the small droplet size and the large surface area of the droplets produced by ultrasonic agitation or a compressed air atomizer, the combined wet electrostatic precipitator and droplet generator described above will have excellent gas absorptive properties, and can be used as a combined gas and particle scrubber. The combined gas and particle scrubber will have a variety of applications in air pollution control. For instance, in the semiconductor industry, the exhaust gas from the vacuum pump downstream of a semiconductor process equipment often contains both toxic gases as well as fine particulate matter. One such gas is fluorine, which is used at the end of a process cycle to clean the process chamber. Fluorine is very reactive to water and will be efficiently scrubbed by water droplets in the combined droplet generator and wet electrostatic precipitator. Similarly, various acidic vapors such as hydrogen fluoride (HF) and hydrogen chloride (HCl) can be absorbed by water droplets or by an aqueous solution of KOH and other basic solutions. By combining a droplet generator with appropriate chemical scrubbing solutions and the wet electrostatic precipitator, a highly efficient combined gas and particle scrubber can be obtained.
In this two-stage design, the relatively short corona wire lengths 113A forming electrodes produce a corona discharge to charge the droplets or particles moving past the corona-discharge electrode 102. The short length of electrode 102 reduces the corona output from the wires, hence the required current output from the power source 106 is reduced, in turn reducing its physical size, and cost. The design also makes it possible to vary the radius of the circle of the corona wire lengths 113A independently from that of the radius of the tubular cylinder electrode 104. By changing these two radii, both the corona discharge electrode 102, which is an ionizer, and the precipitating cylinder electrode 104 can be independently optimized, leading to improved overall operation of the system.
The discs 108 and 110 are held together with a central support 112. The fine wire 113 is threaded between the discs 108 and 110, and carries the high voltage from the source 106. The high voltage again is carried by wire through an insulator bushing 118, which is surrounded by high voltage carrying shield 120. An end plate 104A on tube 104 carries the voltages to the tube 104. The tube 104 in turn is connected to the disc 108 for powering the corona discharge electrode 102. The flow of gas is from an inlet 116 of housing 12 to an outlet 117, which discharges clean gas.
The compact electrostatic precipitator described herein can be used to remove suspended particles in the blowby gas from a diesel engine or other internal combustion engines. The blowby gas with the suspended particulate matter removed can be discharged directly into the atmosphere, or can be recirculated into the engine.
This T-connector constitutes a crankcase pressure regulating device when an electrostatic precipitator is used to remove particles from the blowby gas for recirculation into the diesel intake. Its operation is as follows. The T-connector 138 inlet 138B is open to the atmosphere, and thus the outlet of the precipitator 137 is also at atmospheric pressure. The crankcase pressure Pc relative to atmospheric pressure Pa is thus Pc−Pa=ΔP, where ΔP is the pressure drop of the blowby gas through the precipitator 137. This pressure drop is usually quite low, on the order of a few inches of water or less. The crankcase pressure is thus limited to a few inches of water above atmospheric. In an internal combustion engine, the crankcase pressure must not be allowed to vary by more than a few inches above or below atmospheric to prevent leakage of crankcase oil to the outside, and other operational difficulties. This design makes it possible to achieve crankcase pressure regulation with a simple connection and at low cost.
In a diesel engine using a turbo-charger or turbo-compressor to increase the engine power output, as shown in
Alternatively, as shown in
In both the arrangements shown in
To automatically remove this accumulated oil from the intercooler 146, an oil sump 148 is provided in the intercooler to allow the condensed oil to flow into the sump by gravity. The airflow from the intercooler 134 is directed through a flow restriction 150, such as a nozzle or an orifice to create a pressure drop to remove the oil from the intercooler 146 and be carried by the airflow into the engine intake. The oil collected in the oil sump 148 can also be fed to the intake manifold 131 of the engine 135, by the back pressure created by the flow restriction 150.
When the hot blowby gas is directed this way into the filter intake 154, the oil vapor will be quickly cooled as it comes in contact with the cool collecting filter elements of the filter 144. The vapor will thus condense and be collected in the filter housing. At the same time, all submicron size particles, which may not be completely removed by the electrostatic precipitator, will also be subjected to the strong thermophoretic forces created by the temperature gradient in the boundary layer of the gas flow around the collecting elements of the filter 144. This thermophoretic force can be effectively utilized to remove these submicron particles. Normal engine intake air filters are designed to collect particles larger than a few micron in diameter only. Small particles in the submicron size range are usually not collected. By utilizing the thermophoretic force, the fine particles in the blowby gas can also be collected, thus making the incoming air to the turbo-charger cleaner. With proper design, oil and fine particle accumulation in the intercooler can be reduced to very low level.
This action increases the back pressure in the oil sump and forces the collected oil out a line 161 to the intake manifold 131 of the diesel engine. The solenoid controlled restrictor can be any desired form, such a as a valve that closed partially, or an orifice that is introduced into the flow passageway.
The support sleeve 206A has an open center, and an end insulator portion 215 of a main electrode support 212 is mounted therein. The upper end insulator portion 215 of the support 212 is supported on the cover 208 in a suitable manner. The upper end insulator portion has a receptacle for a heater assembly 216, which has heaters 218 mounted in a outer jacket 219 that is heat conducting and in contact with the insulator portion 215. The outer jacket 219 can be made of copper, which is a very good heat conductor, to distribute the heat uniformly to its outer surface and keep the insulator surface 213 hot and clean from contamination by vapor condensation and particle deposition. The top plate 220 is a heat insulator to reduce the heating power required to operate the heater. The electrical power to operate the heater, usually 12 or 24 volts, is carried by the electrical leads 221 passing through the top plate 220.
A power connection line 224 can be passed out through a central opening of a cap 222. As shown, a power supply 226 to provide the high voltage for the discharge electrode can be potted in the cap 222 and the connector line or rod 225 can be within the precipitator and does not have to extend through the cap. The line 224 can be a relatively low voltage, for example, a 24-volt supply could be provided. The heaters 218 also would be connected generally to a 24-volt supply.
The main support 212 includes a hollow center electrode support 214 that can be, for example, injection molded as a single piece with the main support 212. The electrode support 214 has an interior passageway in which the high voltage connection rod or line electrode 225 extends, and a thin electrode wire 227 can extend for connection directly to the electrode wire shown at 228 that, as shown, is helically wrapped around the insulating support 214. The electrode wire 228 is shown larger than actual size and is a thin wire as previously explained. The insulating material sleeve 214 may be attached to the main support 212 with suitable screws threaded up into the support 212. The upper part of the insulating support has a conducting sleeve 217, which can be made of a metal and connected to the same high voltage electrode wire 226. The insulating support 214 can have a cross section that is cylindrical, if desired, or as shown in
The cross section can take any desired configuration, as long as the spacings are maintained for a corona discharge.
The aerosol flow would come in as shown by the arrow 234, and flow up and around the passageway 235 between the high-voltage electrode wire 228 and the collector electrode 200. In this case, the collector electrode 200 is not a porous member, but is a solid member that can either be stainless steel, for example, or could be a conducting plastic. As the flow passes through the space between the electrode wire 228 and the collector 200, the particles are charged by the corona ions produced by the wire electrode 228. Some of these particles are precipitated onto the collector 200 in this region. The remaining particles are carried by the gas to the upper part of the assembly between the precipitator electrode 217 and the collector electrode 220, where they are precipitated onto the collector 220 by virtual of the high voltage on the electrode 217. The flow then goes up through the openings 204, and out through the outlet 203 as shown. The main support 212 and the electrode support 214 can be injection molded as a single piece, if desired, with conductors formed as slip-fit jackets, or wrapped wires. The heaters 218 are easily installed to maintain the temperature of the insulator at a desired level.
The high temperature at the heaters keeps vapor that enters the space between the sleeve 206A and the upper high voltage insulator portion 215 from condensing on the surface 213 of the high voltage insulator portion 215 in the region around the center portion 215. The heaters also provide enough heat to tend to repel contaminant particles by the thermophoretic effect and prevent them from depositing on the surface 213 of the high voltage insulator portion 215. The heaters 218 are in heat transfer, contacting relation to the insulator portion 215 and will maintain the temperature of the surface 213 sufficiently high to prevent contaminant particles from building up on the surface of the insulator portion. Preferably the temperature of the surface 213 of the insulator portion 215 is 10.degree. or more than the temperature of the gas in the vicinity of the insulating surface 213 inside the precipitator housing.
One such pattern for the wire 252 is shown in
Another way of fabricating the thin wire discharge electrode is to use a flat, thin dielectric, generally plastic, having a thin film clad on the outer surface. The flat thin dielectric with a thin film on the outer surface can be similar to those used in fabricating flexible, electric circuit boards. The electrode wire pattern on the surface can be etched by photolithography. The thin film forming the pattern can then be applied to the surface of the support structure by an adhesive. In such a case, the wire will no longer have a circular cross section. The lateral dimension of the etched electrode, however, must be sufficiently small to sustain a corona discharge at the applied high voltage material.
The compact electrostatic precipitators shown are intended primarily for droplet aerosol collection. The high collection efficiency for the compact size also make the precipitators suitable for collecting dry particle aerosols. The collected dry particles will accumulate in the unit and the precipitators must be periodically shut down for cleaning and maintenance. This is usually acceptable for most applications.
The compact electrostatic precipitator described herein, though not necessary for the application, is particularly attractive because of its compact physical size and high collection efficiency.
Lid 314 has first and second distally opposite faces 316 and 318. Face 316 faces axially outwardly away from canister 302. Face 318 faces axially inwardly into canister 302. Corona discharge electrode assembly 304 is mounted to lid 314 by an insulator 320 extending along face 318. Insulator 320 is axially between face 318 and power supply 308. Insulator 320 has first and second distally opposite faces 322 and 324. First face 322 of insulator 320 faces axially toward and engages second face 318 of lid 314. Second face 324 of insulator 320 faces axially inwardly into canister 302. Hollow interior 306 of corona discharge electrode assembly 304 extends from second face 324 of insulator 320 axially inwardly into the canister. Power supply 308 faces second face 324 of insulator 320 and extends axially inwardly in hollow interior 306. Power supply 308 and hollow interior 306 are on the second face side 324 of insulator 320 opposite the first face side 322 of the insulator. The power supply is conventional and includes conventional transformer circuitry for stepping up the voltage, e.g. from a 12 or 24 volt DC input at 326 to a high voltage output at 328, such as several thousand volts, e.g. 15 kV, connected to corona wire 305. It is preferred that the power supply include a low voltage circuit board for a 12 or 24 volt DC input, also providing a monitoring circuit, connected by lead 332 to a high voltage circuit board 334, as is standard. It is further preferred that the circuit boards be potted with electrical potting compound 336 in hollow interior 306 of corona discharge electrode assembly 304. Low voltage lead 326 extends axially through lid 314 and axially through insulator 320. The low voltage lead preferably includes a plurality of conductors and respective connection pins therefor, such as a first connection pin 338 for feeding 12 or 24 volts DC from a voltage source, such as the battery or electrical system of the vehicle, a second pin 340 providing the low voltage ground, and a third pin 342 providing a power supply diagnostic.
In one embodiment, corona discharge electrode assembly 304 is provided by a plastic insulating bobbin 344 extending axially between first and second axial ends 346 and 348. Bobbin 344 has an inner surface 350 defining hollow interior 306, and has an outer surface 352 facing canister 302 and spaced inwardly therefrom. Corona discharge conductor 305 extends along outer surface 352 and is spaced radially outwardly thereof as above. Canister 302 is grounded, as is known, and provides an annular ground plane providing the collector electrode as above. First axial end 346 of bobbin 344 is mounted to second face 318 of lid 314, in any suitable manner, such as sonic welding, adhesive bonding, etc., and provides the noted insulator.
Precipitator 300 is preferably used in a diesel engine electrostatic crankcase ventilation system as above, for blowby gas. Housing 354 has an inlet 356 as above for receiving blowby gas from the diesel engine, and has an outlet 358 as above for discharging the blowby gas after removal of suspended particulate matter including oil droplets from the blowby gas, and returning the blowby gas to diesel engine as above, to the fresh air intake of the diesel engine, for example a turbocharger or compressor, thus providing blowby gas recirculation. Precipitated oil droplets drain from the housing at drain 357 back to the oil pan of the engine, as above. Housing 354 includes axially extending canister 302 having open axial end 312 closed by lid 314. The lid may include a disc or plate portion 360 having a plurality of apertures 362 providing flow distribution therethrough into the upper plenum space of the canister prior to discharge of the gas at outlet 358, comparably to above noted disc or plate 206 and apertures 204.
Insulator 320 is axially aligned with hollow interior 306 and axially spaces power supply 308 from lid 314 and is disposed axially inwardly of open axial end 312 of the canister. Low voltage lead 326 extends axially through first and second faces 316 and 318 of lid 314 and axially through first and second faces 322 and 324 of insulator 320.
The invention provides an electrostatic precipitator 300 including a housing 354, a corona discharge electrode assembly 304 in the housing, an insulator 320 extending along an inner surface 318 of a wall 314 of the housing, a power supply 308 in the housing on the opposite side 324 of the insulator from the housing wall 314 such that insulator 320 is between housing wall 314 and power supply 308, and a low voltage lead 326 extending through the housing wall 314 and through the insulator 320 to the power supply 308, the power supply 308 supplying high voltage for the corona discharge electrode assembly 304. The housing is preferably provided by a canister 302 closed by a lid 314, with the lid providing the noted housing wall having the noted internal surface 318 along which insulator 320 extends, and with the low voltage lead 326 extending through lid 314 and insulator 320. Canister 302 has the noted open end 312 closed by lid 314, and the power supply 308 is recessed in the housing inwardly of open end 312. Power supply 308 is spaced from lid 314 by insulator 320 therebetween.
It is recognized that various equivalents, alternatives and modifications are possible within the scope of the appended claims.
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| Number | Date | Country | |
|---|---|---|---|
| 20040226449 A1 | Nov 2004 | US |
