US3378725A - Electron capture detector having separate ionization and sensing regions - Google Patents

Electron capture detector having separate ionization and sensing regions Download PDF

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US3378725A
US3378725A US359827A US35982764A US3378725A US 3378725 A US3378725 A US 3378725A US 359827 A US359827 A US 359827A US 35982764 A US35982764 A US 35982764A US 3378725 A US3378725 A US 3378725A
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cathode
anode
discharge
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chamber
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Julius H Bochinski
James C Sternberg
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Beckman Coulter Inc
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Beckman Instruments Inc
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01JELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J41/00Discharge tubes for measuring pressure of introduced gas or for detecting presence of gas; Discharge tubes for evacuation by diffusion of ions
    • H01J41/02Discharge tubes for measuring pressure of introduced gas or for detecting presence of gas
    • H01J41/06Discharge tubes for measuring pressure of introduced gas or for detecting presence of gas with ionisation by means of cold cathodes
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N30/00Investigating or analysing materials by separation into components using adsorption, absorption or similar phenomena or using ion-exchange, e.g. chromatography or field flow fractionation
    • G01N30/02Column chromatography
    • G01N30/62Detectors specially adapted therefor
    • G01N30/64Electrical detectors
    • G01N30/70Electron capture detectors

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  • An anode and cathode are positioned in the sensing portion having a gradient established thereacross not exceeding approximately .7 of a volt per centimeter per millimeter of mercury pressure therebetween to provide for electron capture operation.
  • a sample gas contained in a carrier inactive with respect to the sample and having no electron capture capability, flows past the anode into the sensing portion and is exhausted from a point between the anode and cathode together with the inert gas from the discharge portion.
  • This invention relates to a detector for use in gas chromatography and more particularly to an improved form of such a detector adapted to operate in the electron capture mode.
  • detectors have been used in the prior art in gas chromatography such as thermal conductivity, hydrogen flame, solution conductivity, breakdown voltage and photoelectric effect detectors, detectors employing radioactive materials for ionization, etc.
  • Electron capture detectors heretofore employing radioactive isotopes as a source of ionization, have been widely used in the analysis of electroncgative materials such as pesticides, steroids and amino acids. These detectors are particulariy advantageous because of their great sensitivity and high degree of selectivity.
  • the radioactive isotopes present both health hazards and require government licenses, requiring specialized handling.
  • the upper operating temperatures of such detectors have been a serious limitation, for example where more sensitive detectors have employed tritium sources. Tritium employed in detector structure vaporizes appreciably above 220 C, Accordingly, it is an object of this invention to provide an electron capture detector which does not employ radioactive isotopes.
  • Another object of the invention is to provide such a detector having an upper operating temperature limited only by the materials of construction, for example 400 to 500 C.
  • Still another object of the invention is to provide such a detector in which the source of ionization is a combination of electric discharge and ultraviolet light.
  • a further object is to provide such a detector employing ceramic and metal body portions to permit operation at higher temperatures.
  • a still further object of the invention is to provide such a detector in which the electron current may be varied over several orders of magnitude and which may operate at current levels greatly exceeding those presently available in detectors employing radioactive sources.
  • a chamber having a discharge portion with a pair of discharge electrodes and a sensing portion.
  • An apertured anode and cathode are positioned in the sensing portion and a restriction is provided connecting the two portions of the chamber.
  • a source of potential to establish a gradient not exceeding .7 of a volt per centimeter per millimeter of mercury pressure, is connected across the anode and cathode and a second source is connected to create a discharge across the discharge electrodes.
  • a gas which is chemically inert with respect to the materials of the detector and its other contents is injected into the discharge portion to flow past the dis-charge electrodes through the restriction and then through the cathode.
  • a carrier gas which may contain a sample gas capable of capturing electrons is injected through the anode into the sensing chamber.
  • the two gases are exhausted from a point between the cathode and anode.
  • the relative potential of the electrodes is set such that the discharge electrode field is negative and the anode positive with respect to the cathode to enhance the flow of electrons from the discharge electrodes into the sensing portion of the detector.
  • Typical gases which may be used in the discharge portion are hydrogen, nitrogen, carbon dioxide and the noble gases.
  • carrier gases examples are carbon dioxide, nitrogen and a mixture of the noble gases and others such as argon and methane.
  • a detector having a cylindrical sensing chamber 10 contained in a cylindrical housing 12 which may be made from alumina, for example. Opposite ends of the sensing portion 10 are defined by a cathode 14 and an anode 16 which may be made of stainless steel mesh (approximately 200 mesh).
  • the chamber 10 may be approximately A2 inch in diameter and ,3 inch from the anode to the cathode and has an exhaust port 18 which may be approximately /s inch OD. and positioned about /3 of the way from the cathode to the anode.
  • An inlet port 20 is provided for passing carreir gas, which may contain a sample, through the anode 16 into the sensing chamber 10.
  • a lead 22 is taken from the cathode 14 through the housing 12 to provide an electrical connection to a source of potential 24 and thence to ground.
  • a second lead 26 is taken from anode 16 through housing 12 to provide an electrical connection to an amplifier 23 and then to a recorder 30. Potential source 24 thus establishes the required gradient between the anode 16 and the cathode 14.
  • the housing 12 is attached to a housing 32, which may be of stainless steel, by means of a cylindrical collar 34, which may be made of nickel.
  • Housing 32 has inserted within it an inner housing 36, which may be of quartz or ceramic, which defines a discharge chamber 38.
  • Discharge chamber 38 contains two discharge electrodes 40 which may have platinum tips of approximately .03 inch in diameter spaced approximately .03 inch apart.
  • the discharge electrodes 48 are sealed in bushings 42 which may be of alumina or cezamic and electrodes: 40 may be approximately inch from cathode 14.
  • Bushings 42 each have a collar 44, which may be of nickel, on top of which a gasket 46, which may be of silver, is placed. A seal is provided by screwing the retaining nuts 48, which may be of steel, down on the gaskets 46.
  • the inner housing 36 is held in place in the housing 32 by means of a gasket 50 which may be of silver and a back-up plate 52 which may be of stainless steel.
  • a second back-up plate 5'4 which may also be of stainless steel, forces back-up plate 52 against gasket 5 and is held in place by means of screws 56 which pass through housing 32.
  • a tube 58 is inserted in back-up plate 52 and provides an inlet port which extends through the back-up plate 52 and washer 50 and through housing 36 into the discharge chamber 38, through which a gas for the discharge chamber, such as hydrogen, nitrogen, carbon dioxide or a noble gas may be admitted.
  • the discharge chamber 38 may have dimensions of approximately .18 inch in drameter by .36 inch long.
  • a flow path is provided through a restriction 60 which may be approximately .7 inch in diameter, from the discharge chamber 38 and through an intervening space 62 between the discharge chamber 38 and the sensing chamber 10 of the detector, such that the gas sweeping through tube 58 may pass the discharge electrodes 40 in the chamber 38 and sweep electrons through the restriction 60 into the sensing chamber 10 past cathode 14.
  • Discharge electrodes 40 are connected together by leads 64 and 66, which pass through the bushings 42, through a source of potential 68 and a resistor 70, which may be for example approximately -40,000 ohms, in order to cause a discharge between the electrodes.
  • the terminal 72 between source of potential 68 and resistor 70 is grounded as shown.
  • the source of potential 68 may be approximately 200 to 400 volts, when using helium as a discharge chamber gas; and source 24 may range from 0 to 500 volts for example with polarities as indicated.
  • a gradient is established across the anode 16 and cathode 14 of less than approximately .7 of a volt per centimeter per millimeter of mercury pressure in the chamber which may operate around atmospheric pressure. This is done in order to operate in the electron capture mode avoiding electron multiplication.
  • the flow of gas past the discharge electrodes 40 and through the restriction 60 serves to prevent the carrier gas, containing any sample, flowing through port 20 from coming into contact with the platinum-tipped discharge electrodes 40.
  • the relative potentials of the field between the discharge electrodes 40, cathode 14 and anode 16 serve to accelerate electrons generated in the are at discharge electrodes 40 through cathode 14 to anode 16 where they are collected.
  • Resistor 70 is employed specifically to accomplish this by establishing the discharge electrode nearest ground potential also negative with respect to the cathode 14.
  • An additional effect taking place within the detector occurs in that photons generated at the discharge electrodes 40 radiate through the restriction 60 and strike the cathode 14 releasing additional electrons.
  • the flow of gas from the discharge chamber 38 through the cathode 14 also serves to prevent contamination and modification of the cathode 14 with respect to its photoelectric emission properties.
  • Helium is one preferred gas used in the discharge chamber 38 because of the relatively low potential required to strike an arc.
  • a preferred carrier gas for the sensing chamber is nitrogen which is made to flow counter to the stream of electrons passing between cathode 14 and anode 16.
  • electronegative materials such as pesticides, steroids and amino acids that exhibit the property of capturing some of the electrons out of the flow are contained in the nitrogen, the electron flow, the density of which may be conveniently modified by controlling the applied potentials, is diminished.
  • the decrease in the electron current flowing between cathode 14 and anode 16 yields an indication of the type, presence and amount of electronegative sample gas contained in the carrier when calibrated with time after injection of the sample into a chromatograph column which is thus indicated by a reduction in the current passing through the amplifier 28 and resulting variation recorded on the recorder 30.
  • the suggested materials of construction also permit operation of the detector at temperatures up to 400 to 500 C., which is ab ve t e column peratures normally employed. The detector then can operate in an oven to avoid condensation of sample.
  • An electron capture detector comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge por tion, means for connecting a source of potential across said discharge electrodes, an anode and a cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a gas chemically inert with respect to the detector and its other gas contents into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a carrier gas for containing a sample into said sensing portion to flow past said anode, said carrier gas being inactive with respect to said sample and having substantially no electron capture capability, and means for exhausting said gases from a point between said anode and cathode.
  • An electron capture detector for a gas chromatog raph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential across said discharge electrodes, an anode and a cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a noble gas into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a carrier gas into said sensing portion to flow past said anode, and means for exhausting said gases from a point between said anode and cathode.
  • An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sufiicient to cause an arc across said discharge electrodes, an apertured anode and an apertured cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a gas chemically inert with respect to the detector and its other gas contents into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a carrier gas for containing a sample gas having an afiinity for electrons into said sensing portion to flow past said anode, said carrier gas being inactive with respect to said sample and having substantially no electron capture capability, means for exhausting said gases from a point between said anode and cathode
  • An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sutficient to cause an arc across said discharge electrodes, an apertured anode and an apertnred cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a noble gas into said discharge portion to flow past said discharge electrode and through said cathode, means for admitting a carrier gas for containing a sample gas having an affinity for electrons into said sensing portion to flow past said anode, means for exhausting said gases from a point between said anode and cathode, and said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode.
  • An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sutficient to cause an arc across said discharge electrodes, an apertured anode and an apertured cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting helium gas into said discharge portion to flow past said discharge electrodes and through said cathode, means for admitting nitrogen gas for containing a sample gas having an afiinity for electrons into said sensing portion to flow past said anode, means for exhausting said gases from a point between said anode and cathode, and said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode.
  • An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sufiicient to cause an arc across said discharge electrodes, an apertured anode and an apertured cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approxmiately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting helium gas into said discharge portion to flow past said discharge electrodes and through said cathode, means for admitting nitrogen gas for containing a sample gas having an aflinity for electrons into said sensing portion to flow past said anode, means for exhausting said gases from a point between said anode and cathode, said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode, and
  • An electron capture detector for a gas chromatograph comprising, a discharge chamber and a sensing chamber, a pair of platinum tipped discharge electrodes positioned in said discharge chamber, means for connecting a source of potential sufficient to cause an arc across said discharge electrodes, an anode of stainless steel mesh positioned in said sensing chamber, a cathode of stainless steel mesh positioned across one end of said sensing chamber, a necked down chamber connecting said discharge and sensing chambers, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a helium gas into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a mixture of nitrogen and a sample gas having an afiinity for electrons into said sensing portion to first flow past said anode, means for exhausting said gases from a point between said anode and cathode such that said mixture

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Description

P 1968 J. H. BOCHINSKI ETAL 3,378,725
ELECTRON CAPT URE DETECTOR HAVING SEPARATE IONIZATION AND SENSING REGIONS Filed April 15, 1964 A n 1 ll] WA \YN II/l),
5:, I fiifi jgfikngm s2 II /34 40 32 22 I ZO 3O RECORDER -l INVENTORS JULIUS aeocumsm JAMES c. STERNBERG T: MUM
ATTORNEY United States Patent 3,378,725 ELECTRON CAPTURE DETECTOR HAVING SEP- ARATE IONIZATION AND SENSING REGICNS Julius H. Bochinski, Fasadena, and James C. Sternberg, Fullerton, Calif., assignors to Beckman Instruments, Inc., a corporation of California Filed Apr. 15, 1964, Ser. No. 359,827 7 Claims. (Cl. 315-111) ABSTRACT OF THE DISCLOSURE An electron capture detector for use such as in gas chromatography having separate ionization and sensing portions with discharge electrodes and a gas chemically inert with respect to the detector in the discharge portion. An anode and cathode are positioned in the sensing portion having a gradient established thereacross not exceeding approximately .7 of a volt per centimeter per millimeter of mercury pressure therebetween to provide for electron capture operation. A sample gas contained in a carrier, inactive with respect to the sample and having no electron capture capability, flows past the anode into the sensing portion and is exhausted from a point between the anode and cathode together with the inert gas from the discharge portion.
This invention relates to a detector for use in gas chromatography and more particularly to an improved form of such a detector adapted to operate in the electron capture mode.
Many different forms of detectors have been used in the prior art in gas chromatography such as thermal conductivity, hydrogen flame, solution conductivity, breakdown voltage and photoelectric effect detectors, detectors employing radioactive materials for ionization, etc. Electron capture detectors, heretofore employing radioactive isotopes as a source of ionization, have been widely used in the analysis of electroncgative materials such as pesticides, steroids and amino acids. These detectors are particulariy advantageous because of their great sensitivity and high degree of selectivity. However, the radioactive isotopes present both health hazards and require government licenses, requiring specialized handling. Also, the upper operating temperatures of such detectors have been a serious limitation, for example where more sensitive detectors have employed tritium sources. Tritium employed in detector structure vaporizes appreciably above 220 C, Accordingly, it is an object of this invention to provide an electron capture detector which does not employ radioactive isotopes.
Another object of the invention is to provide such a detector having an upper operating temperature limited only by the materials of construction, for example 400 to 500 C.
Still another object of the invention is to provide such a detector in which the source of ionization is a combination of electric discharge and ultraviolet light.
A further object is to provide such a detector employing ceramic and metal body portions to permit operation at higher temperatures.
A still further object of the invention is to provide such a detector in which the electron current may be varied over several orders of magnitude and which may operate at current levels greatly exceeding those presently available in detectors employing radioactive sources.
In carrying out the invention in one form thereof a chamber is provided having a discharge portion with a pair of discharge electrodes and a sensing portion. An apertured anode and cathode are positioned in the sensing portion and a restriction is provided connecting the two portions of the chamber. A source of potential, to establish a gradient not exceeding .7 of a volt per centimeter per millimeter of mercury pressure, is connected across the anode and cathode and a second source is connected to create a discharge across the discharge electrodes. A gas which is chemically inert with respect to the materials of the detector and its other contents is injected into the discharge portion to flow past the dis-charge electrodes through the restriction and then through the cathode. A carrier gas which may contain a sample gas capable of capturing electrons is injected through the anode into the sensing chamber. The two gases are exhausted from a point between the cathode and anode. The relative potential of the electrodes is set such that the discharge electrode field is negative and the anode positive with respect to the cathode to enhance the flow of electrons from the discharge electrodes into the sensing portion of the detector. Typical gases which may be used in the discharge portion are hydrogen, nitrogen, carbon dioxide and the noble gases. For carrier gases examples are carbon dioxide, nitrogen and a mixture of the noble gases and others such as argon and methane.
The novel features which are believed to be characteristic of the invention are set forth with particularity in the appended claims. The invention itself, however, together with further objects and advantages thereof, can best be understood by reference to the following description taken in connection with the accompanying drawing illustrating one embodiment of the invention in cross section.
Turning now to the drawing, a detector is illustrated having a cylindrical sensing chamber 10 contained in a cylindrical housing 12 which may be made from alumina, for example. Opposite ends of the sensing portion 10 are defined by a cathode 14 and an anode 16 which may be made of stainless steel mesh (approximately 200 mesh). The chamber 10 may be approximately A2 inch in diameter and ,3 inch from the anode to the cathode and has an exhaust port 18 which may be approximately /s inch OD. and positioned about /3 of the way from the cathode to the anode. An inlet port 20 is provided for passing carreir gas, which may contain a sample, through the anode 16 into the sensing chamber 10. A lead 22 is taken from the cathode 14 through the housing 12 to provide an electrical connection to a source of potential 24 and thence to ground. A second lead 26 is taken from anode 16 through housing 12 to provide an electrical connection to an amplifier 23 and then to a recorder 30. Potential source 24 thus establishes the required gradient between the anode 16 and the cathode 14.
The housing 12 is attached to a housing 32, which may be of stainless steel, by means of a cylindrical collar 34, which may be made of nickel. Housing 32 has inserted within it an inner housing 36, which may be of quartz or ceramic, which defines a discharge chamber 38. Discharge chamber 38 contains two discharge electrodes 40 which may have platinum tips of approximately .03 inch in diameter spaced approximately .03 inch apart. The discharge electrodes 48 are sealed in bushings 42 which may be of alumina or cezamic and electrodes: 40 may be approximately inch from cathode 14. Bushings 42 each have a collar 44, which may be of nickel, on top of which a gasket 46, which may be of silver, is placed. A seal is provided by screwing the retaining nuts 48, which may be of steel, down on the gaskets 46.
The inner housing 36 is held in place in the housing 32 by means of a gasket 50 which may be of silver and a back-up plate 52 which may be of stainless steel. A second back-up plate 5'4, which may also be of stainless steel, forces back-up plate 52 against gasket 5 and is held in place by means of screws 56 which pass through housing 32. A tube 58 is inserted in back-up plate 52 and provides an inlet port which extends through the back-up plate 52 and washer 50 and through housing 36 into the discharge chamber 38, through which a gas for the discharge chamber, such as hydrogen, nitrogen, carbon dioxide or a noble gas may be admitted. The discharge chamber 38 may have dimensions of approximately .18 inch in drameter by .36 inch long.
A flow path is provided through a restriction 60 which may be approximately .7 inch in diameter, from the discharge chamber 38 and through an intervening space 62 between the discharge chamber 38 and the sensing chamber 10 of the detector, such that the gas sweeping through tube 58 may pass the discharge electrodes 40 in the chamber 38 and sweep electrons through the restriction 60 into the sensing chamber 10 past cathode 14.
Discharge electrodes 40 are connected together by leads 64 and 66, which pass through the bushings 42, through a source of potential 68 and a resistor 70, which may be for example approximately -40,000 ohms, in order to cause a discharge between the electrodes. The terminal 72 between source of potential 68 and resistor 70 is grounded as shown.
The source of potential 68 may be approximately 200 to 400 volts, when using helium as a discharge chamber gas; and source 24 may range from 0 to 500 volts for example with polarities as indicated. With the sources of potential of the magnitudes described, and the other typical dimensions given, a gradient is established across the anode 16 and cathode 14 of less than approximately .7 of a volt per centimeter per millimeter of mercury pressure in the chamber which may operate around atmospheric pressure. This is done in order to operate in the electron capture mode avoiding electron multiplication. The flow of gas past the discharge electrodes 40 and through the restriction 60 serves to prevent the carrier gas, containing any sample, flowing through port 20 from coming into contact with the platinum-tipped discharge electrodes 40. This then prevents the discharge electrodes from becoming contaminated. The relative potentials of the field between the discharge electrodes 40, cathode 14 and anode 16 serve to accelerate electrons generated in the are at discharge electrodes 40 through cathode 14 to anode 16 where they are collected. Resistor 70 is employed specifically to accomplish this by establishing the discharge electrode nearest ground potential also negative with respect to the cathode 14. An additional effect taking place within the detector occurs in that photons generated at the discharge electrodes 40 radiate through the restriction 60 and strike the cathode 14 releasing additional electrons. The flow of gas from the discharge chamber 38 through the cathode 14 also serves to prevent contamination and modification of the cathode 14 with respect to its photoelectric emission properties.
Helium is one preferred gas used in the discharge chamber 38 because of the relatively low potential required to strike an arc. A preferred carrier gas for the sensing chamber is nitrogen which is made to flow counter to the stream of electrons passing between cathode 14 and anode 16. When electronegative materials such as pesticides, steroids and amino acids that exhibit the property of capturing some of the electrons out of the flow are contained in the nitrogen, the electron flow, the density of which may be conveniently modified by controlling the applied potentials, is diminished.
The decrease in the electron current flowing between cathode 14 and anode 16 yields an indication of the type, presence and amount of electronegative sample gas contained in the carrier when calibrated with time after injection of the sample into a chromatograph column which is thus indicated by a reduction in the current passing through the amplifier 28 and resulting variation recorded on the recorder 30. The suggested materials of construction also permit operation of the detector at temperatures up to 400 to 500 C., which is ab ve t e column peratures normally employed. The detector then can operate in an oven to avoid condensation of sample.
While the principles of the invention have now been made clear in the illustrative embodiment, there will be immediately obvious to those skilled in the art many modifications in structure, arrangement, proportions, elements and components used in the practice of the invention and otherwise, which are particularly adapted for specific environments and operating requirements, without departing from these principles. The appended claims are therefore intended to cover and embrace any such modifications that fall within the limits only of the true spirit and scope of the invention.
What is claimed is:
1. An electron capture detector comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge por tion, means for connecting a source of potential across said discharge electrodes, an anode and a cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a gas chemically inert with respect to the detector and its other gas contents into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a carrier gas for containing a sample into said sensing portion to flow past said anode, said carrier gas being inactive with respect to said sample and having substantially no electron capture capability, and means for exhausting said gases from a point between said anode and cathode.
2. An electron capture detector for a gas chromatog raph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential across said discharge electrodes, an anode and a cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a noble gas into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a carrier gas into said sensing portion to flow past said anode, and means for exhausting said gases from a point between said anode and cathode.
3. An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sufiicient to cause an arc across said discharge electrodes, an apertured anode and an apertured cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a gas chemically inert with respect to the detector and its other gas contents into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a carrier gas for containing a sample gas having an afiinity for electrons into said sensing portion to flow past said anode, said carrier gas being inactive with respect to said sample and having substantially no electron capture capability, means for exhausting said gases from a point between said anode and cathode, and said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode.
4. An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sutficient to cause an arc across said discharge electrodes, an apertured anode and an apertnred cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a noble gas into said discharge portion to flow past said discharge electrode and through said cathode, means for admitting a carrier gas for containing a sample gas having an affinity for electrons into said sensing portion to flow past said anode, means for exhausting said gases from a point between said anode and cathode, and said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode.
5. An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sutficient to cause an arc across said discharge electrodes, an apertured anode and an apertured cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting helium gas into said discharge portion to flow past said discharge electrodes and through said cathode, means for admitting nitrogen gas for containing a sample gas having an afiinity for electrons into said sensing portion to flow past said anode, means for exhausting said gases from a point between said anode and cathode, and said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode.
6. An electron capture detector for a gas chromatograph comprising, a chamber having a discharge portion and a sensing portion, a pair of discharge electrodes positioned in said discharge portion, means for connecting a source of potential sufiicient to cause an arc across said discharge electrodes, an apertured anode and an apertured cathode positioned in said sensing portion, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approxmiately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting helium gas into said discharge portion to flow past said discharge electrodes and through said cathode, means for admitting nitrogen gas for containing a sample gas having an aflinity for electrons into said sensing portion to flow past said anode, means for exhausting said gases from a point between said anode and cathode, said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode, and the centers of said anode and cathode and the center point: between said discharge electrodes being substantially in a straight line.
7. An electron capture detector for a gas chromatograph comprising, a discharge chamber and a sensing chamber, a pair of platinum tipped discharge electrodes positioned in said discharge chamber, means for connecting a source of potential sufficient to cause an arc across said discharge electrodes, an anode of stainless steel mesh positioned in said sensing chamber, a cathode of stainless steel mesh positioned across one end of said sensing chamber, a necked down chamber connecting said discharge and sensing chambers, means for connecting a source of potential across said anode and cathode to establish a gradient not exceeding approximately seven tenths volt per centimeter per millimeter of mercury pressure therebetween, means for admitting a helium gas into said discharge portion to flow past said discharge electrodes and said cathode, means for admitting a mixture of nitrogen and a sample gas having an afiinity for electrons into said sensing portion to first flow past said anode, means for exhausting said gases from a point between said anode and cathode such that said mixture remains substantially out of contact with said cathode to avoid contamination of said cathode, said sources of potential establishing the field between said discharge electrodes negative and said anode positive with respect to said cathode, and the centers of said anode and cathode and the center point between said discharge electrodes being sub stantially in a straight line.
References Cited UNITED STATES PATENTS JAMES W. LAWRENCE, Primary Examiner. STANLEY D. SCI-ILOSSER, Examiner. R. JUDD, Assistant Examiner.
US359827A 1964-04-15 1964-04-15 Electron capture detector having separate ionization and sensing regions Expired - Lifetime US3378725A (en)

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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3445757A (en) * 1965-10-14 1969-05-20 Mc Donnell Douglas Corp Capillary ionization gas detector and analyzer using timed interval current fluctuations
US3566107A (en) * 1967-11-24 1971-02-23 Hewlett Packard Co Nickel 63 electron capture detector
US3611013A (en) * 1970-02-09 1971-10-05 Westinghouse Electric Corp Breakdown potential control assembly for gas flow-through electrical discharge device
US4063156A (en) * 1976-02-27 1977-12-13 Varian Associates, Inc. Assymetric cylinder electron capture detector
EP0015495A1 (en) * 1979-02-27 1980-09-17 Hewlett-Packard Company Electron capture detector
US4264817A (en) * 1979-02-27 1981-04-28 Hewlett-Packard Company Coaxial electron capture detector with thermionic emission electron source
US4789783A (en) * 1987-04-02 1988-12-06 Cook Robert D Discharge ionization detector
US5317271A (en) * 1991-02-28 1994-05-31 Valco Instruments, Co. High voltage spark excitation and ionization detector system with adjustable sample input for sensitivity control
US5760291A (en) * 1996-09-03 1998-06-02 Hewlett-Packard Co. Method and apparatus for mixing column effluent and make-up gas in an electron capture detector

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Publication number Priority date Publication date Assignee Title
GB810062A (en) * 1956-04-06 1959-03-11 Maurice Elie Nahmias A device to detect smoke
US3174036A (en) * 1961-10-04 1965-03-16 Alexeff Igor Measurement of ultra high vacua by electron bombardment and vacuum ultra violet radiation measurement
US3176135A (en) * 1960-01-26 1965-03-30 Nat Res Dev Apparatus for detecting and analysing low gaseous concentrations
US3247375A (en) * 1960-12-23 1966-04-19 James E Lovelock Gas analysis method and device for the qualitative and quantitative analysis of classes of organic vapors
US3277296A (en) * 1963-03-01 1966-10-04 Wilkens Instr & Res Inc Detection of electronegative compositions by means of electron capture detection

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB810062A (en) * 1956-04-06 1959-03-11 Maurice Elie Nahmias A device to detect smoke
US3176135A (en) * 1960-01-26 1965-03-30 Nat Res Dev Apparatus for detecting and analysing low gaseous concentrations
US3247375A (en) * 1960-12-23 1966-04-19 James E Lovelock Gas analysis method and device for the qualitative and quantitative analysis of classes of organic vapors
US3174036A (en) * 1961-10-04 1965-03-16 Alexeff Igor Measurement of ultra high vacua by electron bombardment and vacuum ultra violet radiation measurement
US3277296A (en) * 1963-03-01 1966-10-04 Wilkens Instr & Res Inc Detection of electronegative compositions by means of electron capture detection

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3445757A (en) * 1965-10-14 1969-05-20 Mc Donnell Douglas Corp Capillary ionization gas detector and analyzer using timed interval current fluctuations
US3566107A (en) * 1967-11-24 1971-02-23 Hewlett Packard Co Nickel 63 electron capture detector
US3611013A (en) * 1970-02-09 1971-10-05 Westinghouse Electric Corp Breakdown potential control assembly for gas flow-through electrical discharge device
US4063156A (en) * 1976-02-27 1977-12-13 Varian Associates, Inc. Assymetric cylinder electron capture detector
EP0015495A1 (en) * 1979-02-27 1980-09-17 Hewlett-Packard Company Electron capture detector
US4264817A (en) * 1979-02-27 1981-04-28 Hewlett-Packard Company Coaxial electron capture detector with thermionic emission electron source
US4304997A (en) * 1979-02-27 1981-12-08 Hewlett-Packard Company Electron capture detector with thermionic emission electron source
US4789783A (en) * 1987-04-02 1988-12-06 Cook Robert D Discharge ionization detector
US5317271A (en) * 1991-02-28 1994-05-31 Valco Instruments, Co. High voltage spark excitation and ionization detector system with adjustable sample input for sensitivity control
US5760291A (en) * 1996-09-03 1998-06-02 Hewlett-Packard Co. Method and apparatus for mixing column effluent and make-up gas in an electron capture detector

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