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US3317790A - Sonic jet ionizer - Google Patents

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US3317790A
US3317790A US52400A US5240060A US3317790A US 3317790 A US3317790 A US 3317790A US 52400 A US52400 A US 52400A US 5240060 A US5240060 A US 5240060A US 3317790 A US3317790 A US 3317790A
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orifice
gas
housing
needle
plate
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Kenneth T Whitby
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University of Minnesota Twin Cities
University of Minnesota System
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01TSPARK GAPS; OVERVOLTAGE ARRESTERS USING SPARK GAPS; SPARKING PLUGS; CORONA DEVICES; GENERATING IONS TO BE INTRODUCED INTO NON-ENCLOSED GASES
    • H01T23/00Apparatus for generating ions to be introduced into non-enclosed gases, e.g. into the atmosphere

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  • This invention relates to apparatus and method for the production of gas ions at normal atmospheric pressure and temperature. More particularly the present invention relates to the ionization of a sonic air jet in a corona and to a sonic jet ionizer device.
  • gas ions may be produced in air at normal atmospheric pressure and temperature by a number of methods, such as heated surfaces, ionizing radiation (radioactive materials), X-rays, ultraviolet light, high frequency electric fields and corona discharge.
  • ionizing radiation radioactive materials
  • X-rays X-rays
  • ultraviolet light high frequency electric fields
  • corona discharge the use of ionizing radiation and a corona discharge are the most practical.
  • the corona discharge method involves the creation of ions by impressing high AC. or DC. voltages on a needle and plate or wire and plate arrangement.
  • corona ionizers are relatively simple and involve less hazards than ionizers employing radioactive isotopes but they are relatively inefficient ion producers. The reason for this is that the same high voltage which produces the ionizing corona is also extremely efiective in collecting the ions. Gas ions have a mobility of about 2 centimeters per second per volt per meter. Thus, in the usual wire and plate ionizer the gas ions are moving at a substantial fraction of the speed of sound and practically all are collected.
  • a sonic jet may be utilized to flush ions, created in the corona between a needle and an orifice in a plate, through the orifice before the ions can be collected on the orifice edge.
  • This system produces ions at a high rate nearing or equalling 100% efficiency and low power consumption.
  • Ion concentrations in the gas jet may be produced which are 100,000 times normal atmospheric levels and 100 times higher than the concentrations which can be produced by any other corona ionizer. This ofliers a two order of magnitude improvement over other known corona ionizers. Positive ions, negative ions or an equal mixture of positive and negative ions can be produced at will.
  • sonic flow will be obtained in an orifice or nozzle when a critical pressure ratio, that is, the ratio of the pressure of a gas at the throat of the nozzle to the upstream pressure, is equal to a critical ratio.
  • a critical pressure ratio that is, the ratio of the pressure of a gas at the throat of the nozzle to the upstream pressure.
  • the principal object of this invention then is to provide a highly efiicient method of producing gas ions in a sonic jet at a low rate of power consumption.
  • Another object of this invention is to provide apparatus for ionizing a sonic gas jet through the corona existing between a needle maintained at high voltage and an orifice plate.
  • FIGURE 1 is a side elevation, in section, of the sonic jet ionizer according to the present invention shown connected schematically to a power source;
  • FIGURE 2 is an end elevation of the ionizing device of FIGURE 1;
  • FIGURE 3 is an enlarged fragmentary partial sectional view showing the relationship between needle and orifice.
  • FIGURE 4 is a transverse section through the ionizer housing showing an alternative means of centering the needle.
  • the illustrated form of ionizer includes a cylindrical housing body 11 enclosed at either end by caps 12 and 13.
  • the cylindrical housing body 11 is formed from an electrically non-conductive material such as, for example, methyl methacrylate tubing sold under the trade names Lucite or Plexiglas and is externally threaded adjacent its ends.
  • Caps 12 and 13 are internally threaded to permit the caps to be screwed on to the ends of the housing body.
  • Cap 12 is provided with a central opening through which a thin wire or red electrode 14 having a needle tip 15 may be passed with a slide fit.
  • the outer surface of cap 12 is provided with a boss 16 through which the central opening extends.
  • a set screw 17 permits the needle electrode to be held tight against longitudinal axial movement.
  • Cap 12 is provided with a further opening into which is fit a gas inlet tube 18 adapted to be connected to a source of gas under pressure, such as compressed air.
  • Cap 13 is provided with a large central opening 19.
  • the cap 13, which thus is in the form of an annular ring, is ctilized to secure a plate 20 in place against the end of tubular housing body 11.
  • Caps 12 and 13 and plate 20 are formed from an electrically conductive material. Plate 20 is desirably of copper or brass.
  • Plate 20 is provided with a small central orifice 21 aligned with the needle electrode tip -15.
  • a bridge structure including a transverse bar 22 disposed spaced from and substantially parallel to the inner surface of plate 20 and supported from the plate by a pair of spacer members 23 and secured to the plate by means of screws 24 or similar attaching means.
  • the bar 22 is provided with an opening into which the needle fits with a slide fit. This opening is in precise alignment with the orifice 21 in order to maintain the alignment of the orifice and the needle tip.
  • the bridge bar and spacers are relatively narrow as shown in FIGURE 2 in order not to substantially interfere with flow of gas through the housing from the gas inlet tube to the orifice.
  • the aligning bridge is composed of electrically non-conductive material, such as methyl methacrylate, in order that the needle may be held out of electrical contact with the plate 20.
  • an alternative means for aligning the needle tip with the plate orifice may be provided by three screws 25 spaced 120 apart around the periphery of a tubular housing 11A.
  • the tip of the needle is spaced from the orifice by a disatnce S, as shown in FIGURE 3 and as defined hereinafter.
  • the orifice 21 is provided with sharp edges.
  • the needle electrode is connected to any suitable high voltage source by means of a connecting conductor 27 and plate 20 is similarly connected through cap 13 and conductor 28, as shown schematically in FIGURE 1.
  • the needel electrode is maintained at between about 2500 and 10,000 volts, and preferably between about 3000 and 5000 volts difierent from the orifice plate.
  • the applied voltage may be alternating current or positive or negative direct current.
  • a variety of high voltage power packs and transformers are commercially available as the power source.
  • Gas is introduced to the ionizer housing through the gas inlet tube at pressures between about 15 and 200 lbs. per square inch gauge and desirably between about 15 and 50 lbs. p.s.i.g. At lower gas pressures low efficiency results with little advantage over existing ionizing devices. Although higher gas pressures may be used't'han the indicated upper limits, no corresponding advantage results.
  • the flow of gas functions to flush the ions through the orifice 21 before they can be collected on the orifice edge.
  • the ions are liberated in the corona at the needle point and are accelerated toward the orifice edge.
  • the sonic gas flow in the orifice passes the ions through the orifice and out with the gas jet with nearly 100% efficiency.
  • the resulting stream of gas ions may be directed for use as desired.
  • Exemplary commercial applications of the ionizer include utilization of the ion jet for the dissipation of processing charges which occur on dielectric materials. These include the dissipation of static chargesoccurring in the processing of plastics and the operation of printing presses and the like, and the prevention of clinging of lint in laundry driers and the like.
  • the high ion concentrations issuing from the ionizer in a high velocity gas jet are in an almost ideal form for dissipating static charges.
  • the jet ionizer can be placed several feet away from the work and perform just as efficiently, or more so, than radioactive ionizers which, because of the extremely rapid neutralization of the ions, require that the ionizers be placed within an inch or less of the surface to be neutralized.
  • the orifice 21 should desirably have a diameter between about 0.0156 and 0.125 inch, that is, between about A,; and inch.
  • the diameter of the needle is not critical but the needle must have a sharp point. It has been determined that the radius of the needle point should be less than about 0.001 inch.
  • the distance S, shown in FIGURE 3, that is, the spacing between the needle point and orifice, should be between about /2 to millimeters.
  • the following is a typical example of the operation of the sonic jet ionizer according to the present invention.
  • An ionizer device substantially as illustrated and described was employed.
  • the diameter of the orifice plate was 1.59 mm., that is, about inch in diameter.
  • the needle tip was spaced from the orifice by a distance of 1.71 mm., that is, just slightly more than A inch.
  • Air was supplied to the air inlet tube at about 30 lbs. per square inch gauge.
  • a negative direct current voltage of 5000 volts was applied to the needle electrode.
  • the ion concentration measured along the axis of the jet ionizer at a distance of about 15 centimeters from the orifice was about 4 10 ions per cubic centimeter.
  • a gas ionizing device for operation under sonic jet fiow conditions comprising a housing, a gas inlet to said housing, said housing including an electrically conductive plate, an orifice centrally disposed in said plate, the diameter of said orifice being between about and inch, said orifice having sharp edges, said orifice providing an ionized gas discharge port from said housing, a pointed needle electrode centrally disposed in said housing, said needle adapted for connection to a high voltage electric power source for applying a high electrical voltage to said needle, said housing being closed save for said gas inlet and orifice, said inlet adapted for connection to a source of gas under pressure sufficient that the ratio of the pressure at the orifice to the inlet gas pressure at least equals the critical pressure ratio for the gas, said needle electrode and orifice plate being electrically insulated from each other and from the housing body, aligning means within said housing spaced from said orifice and electrically insulated from the orifice plate and adapted to hold the a pointed tip of said needle electrode in axial alignment
  • a gas ionizing device for operation under sonic jet 7 flow conditions comprising a housing, a gas inlet to said housing, said housing including an electrically conductive plate, an orifice centrally disposed in said plate, said orifice having sharp edges, said orifice providing an ionized gas discharge port from said housing, a pointed needle electrode centrally disposed in said housing, said needle adapted for connection to a high voltage power source for applying a high electrical voltage to said needle, said housing being closed save for said gas inlet and orifice, said inlet adapted for connection to a source of gas under pressure sufiicient that the ratio of the pressure at the orifice to the inlet gas pressure at least equals the critical pressure ratio for the gas, said needle electrode and orifice plate being electrically insulated from each other and from the housing body, aligning means within said housing spaced from said orifice and electrically insulated from the orifice plate and adapted to hold the pointed tip of said needle electrode in axial alignment with the orifice, the tip of said needle electrode

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Description

W 1957 K. T. WHITBY 3,317,790
SONIC JET IONIZER Filed Aug. 29, 1960 25 To IOKAZ 26 ACmioc I N V EN TOR. KENNETH Z'WH/TBY ATTORNEYJ United States Patent 3,317,790 SONIC JET IONIZER Kenneth T. Whitby, Minneapolis, Minn., assignor to The Regents of The University of Minnesota, Minneapolis, Minn., a corporation of Minnesota Filed Aug. 29, 1960, Ser. No. 52,400 2 Claims. (Cl. 317-4) This invention relates to apparatus and method for the production of gas ions at normal atmospheric pressure and temperature. More particularly the present invention relates to the ionization of a sonic air jet in a corona and to a sonic jet ionizer device. I
In general, gas ions may be produced in air at normal atmospheric pressure and temperature by a number of methods, such as heated surfaces, ionizing radiation (radioactive materials), X-rays, ultraviolet light, high frequency electric fields and corona discharge. Of these, the use of ionizing radiation and a corona discharge are the most practical. However, the use of ionizing radiation is practical only for the production of small quantities of ions and is expensive and involves health hazards when large quantities of ions are required. The corona discharge method involves the creation of ions by impressing high AC. or DC. voltages on a needle and plate or wire and plate arrangement. These corona ionizers are relatively simple and involve less hazards than ionizers employing radioactive isotopes but they are relatively inefficient ion producers. The reason for this is that the same high voltage which produces the ionizing corona is also extremely efiective in collecting the ions. Gas ions have a mobility of about 2 centimeters per second per volt per meter. Thus, in the usual wire and plate ionizer the gas ions are moving at a substantial fraction of the speed of sound and practically all are collected.
It has now been discovered that a sonic jet may be utilized to flush ions, created in the corona between a needle and an orifice in a plate, through the orifice before the ions can be collected on the orifice edge. This system produces ions at a high rate nearing or equalling 100% efficiency and low power consumption. Ion concentrations in the gas jet may be produced which are 100,000 times normal atmospheric levels and 100 times higher than the concentrations which can be produced by any other corona ionizer. This ofliers a two order of magnitude improvement over other known corona ionizers. Positive ions, negative ions or an equal mixture of positive and negative ions can be produced at will.
As is known, sonic flow will be obtained in an orifice or nozzle when a critical pressure ratio, that is, the ratio of the pressure of a gas at the throat of the nozzle to the upstream pressure, is equal to a critical ratio. See, for example, Marks Handbook, 1951 Edition, pages 332 to 334; Engineering Thermodynamics by N. A. Hall and Warren E. Ibele, pages 390 to 394 and Perrys Chemical Engineers Handbook, 1950 Edition, pages 402 and 403. The critical pressure ratio for air is 0.53.
The principal object of this invention then is to provide a highly efiicient method of producing gas ions in a sonic jet at a low rate of power consumption.
It is 'a further object of this invention to provide a method of producing gas ions by passing a gas stream under pressure through a corona between a needle tip and an orifice in a plate.
Another object of this invention is to provide apparatus for ionizing a sonic gas jet through the corona existing between a needle maintained at high voltage and an orifice plate.
Other objects of the invention will become apparent as the description proceeds.
To the accomplishment of the foregoing and related ends, this invention then comprises the features hereinafter fully described and particularly pointed out in the claims, the following description setting forth in detail certain illustrative embodiments of the invention, these being indicative, however, of but a few of the various ways in which the principles of the invention may be employed.
The invention is illustrated by the drawings in which the same numerals refer to corresponding parts and in which:
FIGURE 1 is a side elevation, in section, of the sonic jet ionizer according to the present invention shown connected schematically to a power source;
FIGURE 2 is an end elevation of the ionizing device of FIGURE 1;
FIGURE 3 is an enlarged fragmentary partial sectional view showing the relationship between needle and orifice; and
FIGURE 4 is a transverse section through the ionizer housing showing an alternative means of centering the needle.
Referring now to the drawings, the sonic jet ionizer apparatus is indicated generally at 10. The illustrated form of ionizer includes a cylindrical housing body 11 enclosed at either end by caps 12 and 13. The cylindrical housing body 11 is formed from an electrically non-conductive material such as, for example, methyl methacrylate tubing sold under the trade names Lucite or Plexiglas and is externally threaded adjacent its ends. Caps 12 and 13 are internally threaded to permit the caps to be screwed on to the ends of the housing body.
Cap 12 is provided with a central opening through which a thin wire or red electrode 14 having a needle tip 15 may be passed with a slide fit. The outer surface of cap 12 is provided with a boss 16 through which the central opening extends. A set screw 17 permits the needle electrode to be held tight against longitudinal axial movement. Cap 12 is provided with a further opening into which is fit a gas inlet tube 18 adapted to be connected to a source of gas under pressure, such as compressed air. Cap 13 is provided with a large central opening 19. The cap 13, which thus is in the form of an annular ring, is ctilized to secure a plate 20 in place against the end of tubular housing body 11. Caps 12 and 13 and plate 20 are formed from an electrically conductive material. Plate 20 is desirably of copper or brass.
Plate 20 is provided with a small central orifice 21 aligned with the needle electrode tip -15. In order to hold the needle tip in precise alignment with the orifice there is provided a bridge structure including a transverse bar 22 disposed spaced from and substantially parallel to the inner surface of plate 20 and supported from the plate by a pair of spacer members 23 and secured to the plate by means of screws 24 or similar attaching means. The bar 22 is provided with an opening into which the needle fits with a slide fit. This opening is in precise alignment with the orifice 21 in order to maintain the alignment of the orifice and the needle tip. The bridge bar and spacers are relatively narrow as shown in FIGURE 2 in order not to substantially interfere with flow of gas through the housing from the gas inlet tube to the orifice. The aligning bridge is composed of electrically non-conductive material, such as methyl methacrylate, in order that the needle may be held out of electrical contact with the plate 20.
As shown in FIGURE 4, an alternative means for aligning the needle tip with the plate orifice may be provided by three screws 25 spaced 120 apart around the periphery of a tubular housing 11A.
The tip of the needle is spaced from the orifice by a disatnce S, as shown in FIGURE 3 and as defined hereinafter. As best shown in FIGURE 3, the orifice 21 is provided with sharp edges. The needle electrode is connected to any suitable high voltage source by means of a connecting conductor 27 and plate 20 is similarly connected through cap 13 and conductor 28, as shown schematically in FIGURE 1.
In operation of the ionizer device the needel electrode is maintained at between about 2500 and 10,000 volts, and preferably between about 3000 and 5000 volts difierent from the orifice plate. The applied voltage may be alternating current or positive or negative direct current. A variety of high voltage power packs and transformers are commercially available as the power source.
Gas is introduced to the ionizer housing through the gas inlet tube at pressures between about 15 and 200 lbs. per square inch gauge and desirably between about 15 and 50 lbs. p.s.i.g. At lower gas pressures low efficiency results with little advantage over existing ionizing devices. Although higher gas pressures may be used't'han the indicated upper limits, no corresponding advantage results.
The flow of gas functions to flush the ions through the orifice 21 before they can be collected on the orifice edge. The ions are liberated in the corona at the needle point and are accelerated toward the orifice edge. The sonic gas flow in the orifice passes the ions through the orifice and out with the gas jet with nearly 100% efficiency. The resulting stream of gas ions may be directed for use as desired.
Exemplary commercial applications of the ionizer include utilization of the ion jet for the dissipation of processing charges which occur on dielectric materials. These include the dissipation of static chargesoccurring in the processing of plastics and the operation of printing presses and the like, and the prevention of clinging of lint in laundry driers and the like. The high ion concentrations issuing from the ionizer in a high velocity gas jet are in an almost ideal form for dissipating static charges. The jet ionizer can be placed several feet away from the work and perform just as efficiently, or more so, than radioactive ionizers which, because of the extremely rapid neutralization of the ions, require that the ionizers be placed within an inch or less of the surface to be neutralized.
It has been determined experimentally that for maximum efficiency the orifice 21 should desirably have a diameter between about 0.0156 and 0.125 inch, that is, between about A,; and inch. The diameter of the needle is not critical but the needle must have a sharp point. It has been determined that the radius of the needle point should be less than about 0.001 inch. The distance S, shown in FIGURE 3, that is, the spacing between the needle point and orifice, should be between about /2 to millimeters.
The following is a typical example of the operation of the sonic jet ionizer according to the present invention. An ionizer device substantially as illustrated and described was employed. The diameter of the orifice plate was 1.59 mm., that is, about inch in diameter. The needle tip was spaced from the orifice by a distance of 1.71 mm., that is, just slightly more than A inch. Air was supplied to the air inlet tube at about 30 lbs. per square inch gauge. A negative direct current voltage of 5000 volts was applied to the needle electrode. The ion concentration measured along the axis of the jet ionizer at a distance of about 15 centimeters from the orifice was about 4 10 ions per cubic centimeter. Under the same conditions, but with an applied voltage of positive direct current of 5000 volts, substantially the same ion concentration of positive ions was measured. Under the same conditions, but utilizing 3500 volt alternating current, an ion concentration of more than 1.0 10 per cubic centimeter was measured. The concentrations of ions measured along the axis of the jet ionizer at a distance of about 100 centimeters from the orifice were 6 10 positive ions per cubic centimeter resulting from the use of 5000 volt positive direct current, 4 10 negative ions per cubic centimeter resulting from the use of 5000 volt negative direct current and 2 X 10 mixed ions per cubic centimeter resulting from the use of 3500 volt alternating current.
It is apparent that many modifications and variations of this invention as hereinbefore set forth may be made without departing from the spirit and scope thereof. The specific embodiments described are given by way of example only and the invention is limited only by the terms of the appended claims.
What is claimed is:
1. A gas ionizing device for operation under sonic jet fiow conditions comprising a housing, a gas inlet to said housing, said housing including an electrically conductive plate, an orifice centrally disposed in said plate, the diameter of said orifice being between about and inch, said orifice having sharp edges, said orifice providing an ionized gas discharge port from said housing, a pointed needle electrode centrally disposed in said housing, said needle adapted for connection to a high voltage electric power source for applying a high electrical voltage to said needle, said housing being closed save for said gas inlet and orifice, said inlet adapted for connection to a source of gas under pressure sufficient that the ratio of the pressure at the orifice to the inlet gas pressure at least equals the critical pressure ratio for the gas, said needle electrode and orifice plate being electrically insulated from each other and from the housing body, aligning means within said housing spaced from said orifice and electrically insulated from the orifice plate and adapted to hold the a pointed tip of said needle electrode in axial alignment with the orifice, the tip of said needle electrode having a diameter of less than 0.001 inch, said electrode tip being associated with said orifice and spaced therefrom by about /2 to 10 millimeters to produce a gas-ionizing discharge therebetween upon application of voltage to said needle electrode.
2. A gas ionizing device for operation under sonic jet 7 flow conditions comprising a housing, a gas inlet to said housing, said housing including an electrically conductive plate, an orifice centrally disposed in said plate, said orifice having sharp edges, said orifice providing an ionized gas discharge port from said housing, a pointed needle electrode centrally disposed in said housing, said needle adapted for connection to a high voltage power source for applying a high electrical voltage to said needle, said housing being closed save for said gas inlet and orifice, said inlet adapted for connection to a source of gas under pressure sufiicient that the ratio of the pressure at the orifice to the inlet gas pressure at least equals the critical pressure ratio for the gas, said needle electrode and orifice plate being electrically insulated from each other and from the housing body, aligning means within said housing spaced from said orifice and electrically insulated from the orifice plate and adapted to hold the pointed tip of said needle electrode in axial alignment with the orifice, the tip of said needle electrode being associated with and slightly spaced from said orifice to produce a gas-ionizing discharge therebetween upon application of voltage tosaid needle electrode.
(References on following page) References Cited by the Examine],
UNITED STATES PATENTS Thompson 3 172 Eyler 317-2 Wilner 317-4 Campbell 317-4 Fenn 204--312 Muller et a1. 3172 6 FOREIGN PATENTS 9/1932 Germany. 3/ 1957 Great Britain.
5 MILTON O. HIRSHFIELD, Primary Examiner.
E. JAMES SAX, SAMUEL BERNSTEIN, Examiners.

Claims (1)

1. A GAS IONIZING DEVICE FOR OPERATION UNDER SONIC JET FLOW CONDITIONS COMPRISING A HOUSING, A GAS INLET TO SAID HOUSING, SAID HOUSING INCLUDING AN ELECTRICALLY CONDUCTIVE PLATE, AN ORIFICE CENTRALLY DISPOSED IN SAID PLATE, THE DIAMETER OF SAID ORIFICE BEING BETWEEN ABOUT 1/64 AND 1/8 INCH, SAID ORIFICE HAVING SHARP EDGES, SAID ORIFICE PROVIDING AN IONIZED GAS DISCHARGE PORT FROM SAID HOUSING, A POINTED NEEDLE ELECTRODE CENTRALLY DISPOSED IN SAID HOUSING, SAID NEEDLE ADAPTED FOR CONNECTION TO A HIGH VOLTAGE ELECTRIC POWER SOURCE FOR APPLYING A HIGH ELECTRICAL VOLTAGE TO SAID NEEDLE, SAID HOUSING BEING CLOSED SAVE FOR SAID INLET AND ORIFICE, SAID INLET ADAPTED FOR CONNECTION TO A SOURCE OF GAS UNDER PRESSURE SUFFICIENT THAT THE RATIO OF THE PRESSURE AT THE ORIFICE TO THE INLET GAS PRESSURE AT LEAST EQUALS THE CRITICAL PRESSURE RATIO FOR THE GAS, SAID NEEDLE ELECTRODE AND ORIFICE PLATE BEING ELECTRICALLY INSULATED FROM EACH OTHER AND FROM THE HOUSING BODY, ALIGNING MEANS WITHIN SAID HOUSING SPACED FROM SAID ORIFICE AND ELECTRICALLY INSULATED FROM THE ORIFICE PLATE AND ADAPTED TO HOLD THE POINTED TIP OF SAID NEEDLE ELECTRODE IN AXIAL ALIGNMENT WITH THE ORIFICE, THE TIP OF SAID NEEDLE ELECTRODE HAVING A DIAMETER OF LESS THAN 0.001 INCH, SAID ELECTRODE TIP BEING ASSOCIATED WITH SAID ORIFICE AND SPACED THEREFROM BY ABOUT 1/2 TO 10 MILLIMETERS TO PRODUCE A GAS-IONIZING DISCHARGE THEREBETWEEN UPON APPLICATION OF VOLTAGE TO SAID NEEDLE ELECTRODE.
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US3413545A (en) * 1965-06-23 1968-11-26 Univ Minnesota Apparatus and method for determining aerosol particle concentration and particle size distribution
US3600632A (en) * 1968-12-03 1971-08-17 Technology Uk Static electricity dishcarge systems
US3601649A (en) * 1965-12-13 1971-08-24 Steigerwald Karl Heinz Electron beam generating system for high beam potentials
US3611030A (en) * 1969-10-01 1971-10-05 Herbert Products Ionization apparatus
US3757491A (en) * 1970-11-05 1973-09-11 Gourdine Systems Ins Apparatus for suppressing airborne particles
US4069665A (en) * 1973-08-01 1978-01-24 Scientific Enterprises, Inc. Gas ionizing apparatus for improving the operation of an internal combustion engine
FR2430678A1 (en) * 1978-07-06 1980-02-01 Fleck Carl ION GENERATING APPARATUS
US4228479A (en) * 1978-03-10 1980-10-14 Office National D'etudes Et De Recherches Aerospatiales (O.N.E.R.A.) Device for the production of a gaseous stream carrying electric charges
US4331037A (en) * 1980-06-02 1982-05-25 Tsi Incorporated Fluid flow measuring apparatus
US4339782A (en) * 1980-03-27 1982-07-13 The Bahnson Company Supersonic jet ionizer
EP0051006A3 (en) * 1980-10-14 1983-06-08 Office National D'etudes Et De Recherches Aerospatiales (O.N.E.R.A.) Method and devices to transfer electrical charges of opposed signs into a space-field, and its application to static eliminators
US4394825A (en) * 1980-06-02 1983-07-26 Tsi Incorporated Fluid flow measuring apparatus
US4471654A (en) * 1981-09-25 1984-09-18 Tsi Incorporated Fluid flow measuring apparatus
US4729057A (en) * 1986-07-10 1988-03-01 Westward Electronics, Inc. Static charge control device with electrostatic focusing arrangement
US5877593A (en) * 1994-12-22 1999-03-02 The Secretary Of State For Defence In Her Britannic Majesty's Government Of The United Kingdom Of Great Britain And Northern Ireland Distorted field radio frequency ion source
FR2870082A1 (en) * 2004-05-07 2005-11-11 Valitec Soc Par Actions Simpli STATIC ELECTRICITY ELIMINATOR, IN PARTICULAR FOR THE TREATMENT OF POLYMERS
RU2341918C1 (en) * 2007-06-04 2008-12-20 Государственное образовательное учреждение высшего профессионального образования "Тюменский государственный нефтегазовый университет" Device to remove charges from fluid flow
RU2400021C1 (en) * 2009-07-20 2010-09-20 Государственное образовательное учреждение высшего профессионального образования "Тюменский государственный нефтегазовый университет" Device for charges drain from carbohydrates flow

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US4228479A (en) * 1978-03-10 1980-10-14 Office National D'etudes Et De Recherches Aerospatiales (O.N.E.R.A.) Device for the production of a gaseous stream carrying electric charges
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US4331037A (en) * 1980-06-02 1982-05-25 Tsi Incorporated Fluid flow measuring apparatus
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US5877593A (en) * 1994-12-22 1999-03-02 The Secretary Of State For Defence In Her Britannic Majesty's Government Of The United Kingdom Of Great Britain And Northern Ireland Distorted field radio frequency ion source
FR2870082A1 (en) * 2004-05-07 2005-11-11 Valitec Soc Par Actions Simpli STATIC ELECTRICITY ELIMINATOR, IN PARTICULAR FOR THE TREATMENT OF POLYMERS
WO2005122653A1 (en) * 2004-05-07 2005-12-22 Valitec Static electricity eliminator, particularly for the treatment of polymers
RU2325791C2 (en) * 2004-05-07 2008-05-27 Валитек Device for removing static electricity, in particular, during processing of polymers
US20080278879A1 (en) * 2004-05-07 2008-11-13 Valitec Static Electricity Eliminator, Particularly for the Treatment of Polymers
RU2341918C1 (en) * 2007-06-04 2008-12-20 Государственное образовательное учреждение высшего профессионального образования "Тюменский государственный нефтегазовый университет" Device to remove charges from fluid flow
RU2400021C1 (en) * 2009-07-20 2010-09-20 Государственное образовательное учреждение высшего профессионального образования "Тюменский государственный нефтегазовый университет" Device for charges drain from carbohydrates flow

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