WO1994016320A1 - Method and equipment for definition of foreign matter contents in gases - Google Patents

Method and equipment for definition of foreign matter contents in gases Download PDF

Info

Publication number
WO1994016320A1
WO1994016320A1 PCT/FI1994/000015 FI9400015W WO9416320A1 WO 1994016320 A1 WO1994016320 A1 WO 1994016320A1 FI 9400015 W FI9400015 W FI 9400015W WO 9416320 A1 WO9416320 A1 WO 9416320A1
Authority
WO
WIPO (PCT)
Prior art keywords
gas
led
foreign matter
cell
ions
Prior art date
Application number
PCT/FI1994/000015
Other languages
French (fr)
Inventor
Heikki Paakkanen
Esko KÄRPÄNOJA
Tero KÄTTÖ
Tarmo KARHAPÄÄ
Asko Oinonen
Hannu Salmi
Original Assignee
Environics Oy
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Environics Oy filed Critical Environics Oy
Priority to EP94904196A priority Critical patent/EP0679255A1/en
Publication of WO1994016320A1 publication Critical patent/WO1994016320A1/en

Links

Classifications

    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
    • G01N33/0004—Gaseous mixtures, e.g. polluted air
    • G01N33/0009—General constructional details of gas analysers, e.g. portable test equipment
    • G01N33/0027—General constructional details of gas analysers, e.g. portable test equipment concerning the detector
    • G01N33/0031—General constructional details of gas analysers, e.g. portable test equipment concerning the detector comprising two or more sensors, e.g. a sensor array
    • G01N33/0032—General constructional details of gas analysers, e.g. portable test equipment concerning the detector comprising two or more sensors, e.g. a sensor array using two or more different physical functioning modes

Definitions

  • the invention relates to a method and equipment for defini- tion of foreign matter contents in gas.
  • the most sensitive analysis devices are based on air ioniza- tion, e.g. by alpha- or beta radiation and by measuring the ions in different circumstances.
  • he ions so formed are put to migrate through a particular abyrinth and the remaining ions are measured based on the ci-irent they cause.
  • Another method analyzes the mobility of the formed ions through certain lattices and finally measures the ion current. These two methods generally detect very heavy molecules from the air, like most of the combat gases.
  • the ionized molecules are led through chambers having different electric fields, after which the current is detected from the measuring electrodes, by which the quality and quantity of the foreign matter molecules are identified.
  • the DE-patent publication 2028805 discloses a method for detecting trace vapors, which undergo ion-molecule reactions and for separating, concentrating and measuring of molecular quantities of trace substances in gaseous samples.
  • the detection and measurement is accomplished by utilizing the difference in velocity or drift time of ions of different mass in the electric field applied to the gas stream.
  • the electric field causes the primary ions to migrate towards a plurality of ion gates provided rectangular to the gas stream and in parallel between the electrodes, during which the primary ions react with molecules of a gas to be detect- ed, converting the molecules to secondary or product ions, thereby measuring and classifying the ions according to the particular mass.
  • the CH-publication 550 399 discloses an air pollution mea- suring equipment comprising a first and a second air capaci ⁇ tor each having a suitable length through which ionized air containing pollution flows laminarily at a constant veloci ⁇ ty.
  • the capacitors may have planar or cylindrical electrodes and may comprise two or more electrodes.
  • the electrodes of the capacitors are supplied with different voltages.
  • the output signals measured via the electrodes of the capacitors are applied to the inputs of dividing and summing circuit means, the output of which provide a final output signal which constitutes a measure of air pollution.
  • One of the most important advantages of the invention is that the inaccuracy of the analysis due to gas or air mois ⁇ ture can be eliminated.
  • the reliability of the analysis is improved.
  • the sensitivity is great and the response time is short.
  • Other organic substances or solvents or tobacco smoke do not disturb the foreign matter analysis.
  • Fig. 1 presents a diagram of the measuring equipment of the subject invention.
  • Fig. 2 presents a diagram of another implementation form of the equipment.
  • Fig. 1 presents the equipment according to the invention.
  • the gas to be analyzed is sucked into tube 1, filtered with the heatable filter 2 and led into the ionization cell 3, of which can as such be provided several in parallel or in sequence, and which can either be according to the FI patent 75055 or any gas ionization based gas analysis device, whereafter the gas is led to the semiconductor cell, which can be several in parallel or in sequence.
  • the semiconductor cell can in the solution be any gas sensor based on the reaction between the semiconductor surface and the gas, which as such is based on the known technique.
  • the signals of all measuring cells are utilized simultaneously for the perfor ⁇ mance of the gas analysis for calculations and other conclu ⁇ sions for improved separation of gases from each other in different circumstances.
  • the gas is e.g. charged by the radiation transmitted from the alpha- or beta radiation source 4.
  • the gas is led to a measuring tube 5.
  • the field elec- trodes have the voltage V l V 2 ....V n .
  • the back-plate voltage is V ⁇ .
  • the light ions charged in the gas are collected into the field electrodes V n .
  • the further advanced remaining heavy ions cause an ion current I n to the electrodes in the chamber border, which is registered. From each value I n , in which n is an integer, e.g. 1-6, is formed a diagram, the form of which depicts the substance to be analyzed. Normally the electric field of the ionization cell is stronger in the beginning of the chamber and weaker in the collecting zone.
  • the gas is led further to the semiconductor cell 6, formed of e.g. a tin dioxide(Sn0 2 )crystal.
  • a sensitive analyzing device can be obtained for different substances, e.g. for mustard gas.
  • the signals obtained by the above method and the semiconductor cells are gathered together and analyzed together in e.g. a data processor 7.
  • the gas analyzed by the semiconductor cell together is preferably such a gas, which analyzed as moist, does not give a signal with the above mentioned ionization method but only when measured by the semiconductor cell.
  • An example of such a gas is the mustard gas.
  • the tests for the gas streams having hazardous matter in it have been carried out in different humidities with both the ionization cell and the semiconductor cell mounted sequen ⁇ tially or parallel to each other.
  • the relative humidities were 10, 50 and 90 %.
  • the gas stream was conducted through the channel by a pump.
  • test results show that the presence of the mustard gas will be detected most effectively using the combination of the ionization and semiconductor cell at low concentrations and at all the relative humidities and especially at the moderate or larger humidities.

Landscapes

  • Chemical & Material Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Health & Medical Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Food Science & Technology (AREA)
  • Medicinal Chemistry (AREA)
  • Physics & Mathematics (AREA)
  • Combustion & Propulsion (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Other Investigation Or Analysis Of Materials By Electrical Means (AREA)
  • Sampling And Sample Adjustment (AREA)

Abstract

The object of the invention is a method for detection of foreign matter contents in gas, in which method the gas is led to a flow channel (1), in which the gas is filtered and heated, whereafter the gas is led to the measuring cells (3). The invention is characterized in that for the analyzing of the gas is used at least one ionization cell and at least one semiconductor cell (3, 6) arranged in parallel or in sequence.

Description

METHOD AND EQUIPMENT 1 IR DEFINITION OF FOREIGN MATTER CO TENTS IN GASES
The invention relates to a method and equipment for defini- tion of foreign matter contents in gas.
Foreign matters are analyzed and their contents are defined to control the quality of the breathing air. When defining from the gas certain toxic components which are toxic al- ready in relatively small quantities, other air components may disturb the detection. The contents of different sub¬ stances rapidly and reliably in the air, like carbon diox¬ ide, may vary. The detection of different molecules or molecule groups performed from gases in general " from vapor originating from evaporated solid materia_ or liσu"i matters is often connected with problems. The detection c especially toxic agents in the air, nerve gases diffused in the breathing air, has been a problem due to their small contents. The detections should be made already in a few seconds. The most efficient nerve gases should be detected already at contents of 1/100 ppm.
The most sensitive analysis devices are based on air ioniza- tion, e.g. by alpha- or beta radiation and by measuring the ions in different circumstances. In one method he ions so formed are put to migrate through a particular abyrinth and the remaining ions are measured based on the ci-irent they cause. Another method analyzes the mobility of the formed ions through certain lattices and finally measures the ion current. These two methods generally detect very heavy molecules from the air, like most of the combat gases. In one method the ionized molecules are led through chambers having different electric fields, after which the current is detected from the measuring electrodes, by which the quality and quantity of the foreign matter molecules are identified.
Such a quick and reliable method is presented in the FI- patent 75055. To define the foreign matter contents in the gas in this method, the gas and its components are ionized in the ionization zone. They are led into a narrow analyzer channel, in which they due to the capillary effect have to pass in the middle of the channel. From there they are further deflected by electric fields causing unequal voltag¬ es to the electrode in the channel border, producing there the ion current. By the current spectrum based on ion cur¬ rents, the different substances are identified and the ion contents in the gas is defined by comparing them to corre¬ sponding spectra obtained from standard samples of the different agents. A solution has also been disclosed, in which the ions contained in the gas are, before measuring, separated in a separator into positive and negative ions, of which the other ones are analyzed.
The DE-patent publication 2028805 discloses a method for detecting trace vapors, which undergo ion-molecule reactions and for separating, concentrating and measuring of molecular quantities of trace substances in gaseous samples. In an electric field essentially parallel to the gas stream be¬ tween two electrodes arranged in a detecting chamber, the detection and measurement is accomplished by utilizing the difference in velocity or drift time of ions of different mass in the electric field applied to the gas stream. The electric field causes the primary ions to migrate towards a plurality of ion gates provided rectangular to the gas stream and in parallel between the electrodes, during which the primary ions react with molecules of a gas to be detect- ed, converting the molecules to secondary or product ions, thereby measuring and classifying the ions according to the particular mass.
From the EP-publication 21518 is known a method similar to the one above for detecting trace quantities of chemical species defined in a gaseous mixture by ionizing a propor¬ tion of the molecules and leading these gas molecules through an electric field which is arranged in the above manner in a detecting chamber.
The CH-publication 550 399 discloses an air pollution mea- suring equipment comprising a first and a second air capaci¬ tor each having a suitable length through which ionized air containing pollution flows laminarily at a constant veloci¬ ty. The capacitors may have planar or cylindrical electrodes and may comprise two or more electrodes. In order to provide different electric fields for generating a first and second varying measurement signal as a function of a small and large positive ion concentration in the air stream generated by means of an exhaust fan, the electrodes of the capacitors are supplied with different voltages. The output signals measured via the electrodes of the capacitors are applied to the inputs of dividing and summing circuit means, the output of which provide a final output signal which constitutes a measure of air pollution.
The method and the equipment according to the invention pro¬ vide a decisive improvement of the above presented methods. The implementation of this with the method and equipment according to the invention is mainly characterized in what is presented in claims 1 and 5.
One of the most important advantages of the invention is that the inaccuracy of the analysis due to gas or air mois¬ ture can be eliminated. The reliability of the analysis is improved. The sensitivity is great and the response time is short. Other organic substances or solvents or tobacco smoke do not disturb the foreign matter analysis.
In the following the invention is described with reference to the enclosed drawings, in which:
Fig. 1 presents a diagram of the measuring equipment of the subject invention. Fig. 2 presents a diagram of another implementation form of the equipment.
Fig. 1 presents the equipment according to the invention. The gas to be analyzed is sucked into tube 1, filtered with the heatable filter 2 and led into the ionization cell 3, of which can as such be provided several in parallel or in sequence, and which can either be according to the FI patent 75055 or any gas ionization based gas analysis device, whereafter the gas is led to the semiconductor cell, which can be several in parallel or in sequence.
An alternative solution is to place according to fig. 2, the ionization cells and the semiconductor cells parallel in the gas flow, so that the gas is distributed to be analyzed to both cells /battery.
The semiconductor cell can in the solution be any gas sensor based on the reaction between the semiconductor surface and the gas, which as such is based on the known technique. In the equipment according to the invention the signals of all measuring cells are utilized simultaneously for the perfor¬ mance of the gas analysis for calculations and other conclu¬ sions for improved separation of gases from each other in different circumstances.
The gas is e.g. charged by the radiation transmitted from the alpha- or beta radiation source 4. The gas is led to a measuring tube 5. In the collection field the field elec- trodes have the voltage Vl V2....Vn. The back-plate voltage is Vτ. In the collection field, the light ions charged in the gas, are collected into the field electrodes Vn. In the measuring chamber the further advanced remaining heavy ions cause an ion current In to the electrodes in the chamber border, which is registered. From each value In, in which n is an integer, e.g. 1-6, is formed a diagram, the form of which depicts the substance to be analyzed. Normally the electric field of the ionization cell is stronger in the beginning of the chamber and weaker in the collecting zone.
The gas is led further to the semiconductor cell 6, formed of e.g. a tin dioxide(Sn02)crystal. By changing the doping, a sensitive analyzing device can be obtained for different substances, e.g. for mustard gas. The signals obtained by the above method and the semiconductor cells are gathered together and analyzed together in e.g. a data processor 7. The gas analyzed by the semiconductor cell together, is preferably such a gas, which analyzed as moist, does not give a signal with the above mentioned ionization method but only when measured by the semiconductor cell. An example of such a gas is the mustard gas.
The tests for the gas streams having hazardous matter in it have been carried out in different humidities with both the ionization cell and the semiconductor cell mounted sequen¬ tially or parallel to each other. The relative humidities were 10, 50 and 90 %. The gas stream was conducted through the channel by a pump. In the table, A rresponds ioniza¬ tion cell and B semiconductor cell, respectively.
The following table shows the results of the tests.
Device Conce: ration Humidity Response time which mg/m3 % s responded
B 0,2 90 1 B 0,2 10 9
B 6 90 12
A 6 10 28
B 10 50 9
A 10 10 9
The test results show that the presence of the mustard gas will be detected most effectively using the combination of the ionization and semiconductor cell at low concentrations and at all the relative humidities and especially at the moderate or larger humidities.
The invention has been described with reference to only one of its favorable forms of implementation. The solutions presented above and in the drawings are only examples, and the invention is not to be considered as so limited, but all modifications within the scope of the inventive idea are naturally possible.

Claims

1. A method for detection of foreign matter contents in gases in which the gas stream is ionized at the ionizing zone,
ionized gases and materials contained in the gas stream are led through at least one chamber having different electric fields the fields being transverse to the gas stream, so that at least some ions are removed in the collecting zone in the beginning of the chamber,
the electric currents of the ions reaching the measuring zone are measured in the electric field ,
receiving the signals and on the basis of the amount and relationship of said signals corresponding to the measured electric currents an analysis of the foreign matter in the gases is provided, characterized in that conducting the analyzing gas stream into at least one ionization cell and at least one semicon¬ ductor cell arranged in parallel and/or in sequence to each other.
2. A method for detection of foreign matter contents in gas, in which the gas is led to a flow channel, in which the gas is filtered and heated, whereafter the gas is led to measur¬ ing cells, characterized in that for the analyzing the gas is conducted to at least one ionization cell and at least one semiconductor cell arranged in parallel and/or in sequence.
3. A method according to claim 1 or 2, characterized in that for the analyzing of the gas in different circumstances the signals of the ionization cells and semiconductor cells arranged in parallel or in sequence are utilized simulta¬ neously.
4. A method according to one or more of the above claims, characterized in that the gas is charged and led to a flow channel, the light ions of the gas are removed in the col¬ lection field, and the field currents caused by the heavy ions of the gas are registered.
5. A method according to one or more of the above claims, characterized in that the same gas is further led to the semiconductor cell to detect the presence of some particular substance.
6. An equipment for detection of foreign matter contents in gas, which equipment comprises a flow channel for leading gas to the same, gas filtering and heating devices and measuring cells, characterized in that the measuring cells used for the gas analysis comprise at least one ion¬ ization cell and at least one semiconductor cell arranged in parallel or in sequence.
PCT/FI1994/000015 1993-01-12 1994-01-12 Method and equipment for definition of foreign matter contents in gases WO1994016320A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
EP94904196A EP0679255A1 (en) 1993-01-12 1994-01-12 Method and equipment for definition of foreign matter contents in gases

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
FI930122 1993-01-12
FI930122A FI96903C (en) 1993-01-12 1993-01-12 Method for determining the content of foreign matter in gas and apparatus therefor

Publications (1)

Publication Number Publication Date
WO1994016320A1 true WO1994016320A1 (en) 1994-07-21

Family

ID=8536692

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/FI1994/000015 WO1994016320A1 (en) 1993-01-12 1994-01-12 Method and equipment for definition of foreign matter contents in gases

Country Status (4)

Country Link
EP (1) EP0679255A1 (en)
CA (1) CA2153657A1 (en)
FI (1) FI96903C (en)
WO (1) WO1994016320A1 (en)

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003081224A1 (en) * 2002-03-25 2003-10-02 Lappeenrannan Teknillinen Yliopisto A cell structure, device and methods for gas analysis
DE102005007746A1 (en) * 2005-02-18 2006-08-31 Dräger Safety AG & Co. KGaA Ion mobility spectrometer with parallel drift gas and ion carrier gas flow
EP1724575A1 (en) * 2005-05-20 2006-11-22 Hitachi, Ltd. Gas monitoring apparatus
DE102005031048A1 (en) * 2005-07-02 2007-01-04 Dräger Safety AG & Co. KGaA Ion mobility spectrometer uses unidirectional drift with larger dominant drift gas flow before detector electrode in separation area
DE102007049350A1 (en) 2007-10-15 2009-04-23 Bruker Daltonik Gmbh APCI ion source
DE102008006208A1 (en) 2008-01-26 2009-08-13 Dräger Safety AG & Co. KGaA Gas analysis device i.e. ion mobility spectrometer, for detecting smallest concentration of e.g. drug, has dosing unit operable in dilution operation in which dilution ratio of through flow resistance takes finite value different from zero
DE102008028681A1 (en) * 2008-06-17 2009-12-31 Airbus Deutschland Gmbh Method for operating a metal oxide gas sensor, sensor device for carrying out the method and use thereof
WO2010089375A1 (en) * 2009-02-06 2010-08-12 Eads Deutschland Gmbh Sensor device
WO2011058200A1 (en) 2009-11-11 2011-05-19 Ramem, S.A. Differential mobility analyser

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3342230A1 (en) * 1983-02-21 1984-08-23 Veb Kombinat Robotron, Ddr 8012 Dresden Detector for testing for gases
US5047723A (en) * 1986-06-03 1991-09-10 Pertti Puumalainen Method for detection of foreign matter contents in gases
WO1992010751A1 (en) * 1990-12-06 1992-06-25 Lehmann, Martin Process for the automatic selection of containers amd measuring device therefor and an installation with such a measuring device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3342230A1 (en) * 1983-02-21 1984-08-23 Veb Kombinat Robotron, Ddr 8012 Dresden Detector for testing for gases
US5047723A (en) * 1986-06-03 1991-09-10 Pertti Puumalainen Method for detection of foreign matter contents in gases
WO1992010751A1 (en) * 1990-12-06 1992-06-25 Lehmann, Martin Process for the automatic selection of containers amd measuring device therefor and an installation with such a measuring device

Cited By (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
AU2003216946B2 (en) * 2002-03-25 2009-06-11 Environics Oy A cell structure, device and methods for gas analysis
US7339162B2 (en) 2002-03-25 2008-03-04 Environics Oy Cell structure, device and method for gas analysis
US7586090B2 (en) 2002-03-25 2009-09-08 Environics Ov Cell structure, device and method for gas analysis
WO2003081224A1 (en) * 2002-03-25 2003-10-02 Lappeenrannan Teknillinen Yliopisto A cell structure, device and methods for gas analysis
DE102005007746B4 (en) * 2005-02-18 2009-01-08 Dräger Safety AG & Co. KGaA Ion mobility spectrometer with parallel drift gas and ion carrier gas flow
US7244931B2 (en) 2005-02-18 2007-07-17 Dräger Safety AG & Co. KGaA Ion mobility spectrometer with parallel running drift gas and ion carrier gas flows
DE102005007746A1 (en) * 2005-02-18 2006-08-31 Dräger Safety AG & Co. KGaA Ion mobility spectrometer with parallel drift gas and ion carrier gas flow
US7449685B2 (en) 2005-05-20 2008-11-11 Hitachi, Ltd. Gas monitoring apparatus
EP1724575A1 (en) * 2005-05-20 2006-11-22 Hitachi, Ltd. Gas monitoring apparatus
US7829848B2 (en) 2005-05-20 2010-11-09 Hitachi, Ltd. Gas monitoring apparatus
US7417224B2 (en) 2005-07-02 2008-08-26 Dräger Saftey AG & Co. KGaA Ion mobility spectrometer with parallel drift gas and ion carrier gas flows
DE102005031048A1 (en) * 2005-07-02 2007-01-04 Dräger Safety AG & Co. KGaA Ion mobility spectrometer uses unidirectional drift with larger dominant drift gas flow before detector electrode in separation area
DE102007049350A1 (en) 2007-10-15 2009-04-23 Bruker Daltonik Gmbh APCI ion source
US9214326B2 (en) 2007-10-15 2015-12-15 Bruker Daltonik Gmbh Atmospheric pressure chemical ionization ion source
DE102007049350B4 (en) * 2007-10-15 2011-04-07 Bruker Daltonik Gmbh APCI ion source
DE102008006208B4 (en) * 2008-01-26 2016-05-04 Dräger Safety AG & Co. KGaA Device for gas analysis
DE102008006208A1 (en) 2008-01-26 2009-08-13 Dräger Safety AG & Co. KGaA Gas analysis device i.e. ion mobility spectrometer, for detecting smallest concentration of e.g. drug, has dosing unit operable in dilution operation in which dilution ratio of through flow resistance takes finite value different from zero
DE102008028681A1 (en) * 2008-06-17 2009-12-31 Airbus Deutschland Gmbh Method for operating a metal oxide gas sensor, sensor device for carrying out the method and use thereof
WO2010089375A1 (en) * 2009-02-06 2010-08-12 Eads Deutschland Gmbh Sensor device
WO2011058200A1 (en) 2009-11-11 2011-05-19 Ramem, S.A. Differential mobility analyser

Also Published As

Publication number Publication date
FI96903C (en) 1996-09-10
FI930122A0 (en) 1993-01-12
FI96903B (en) 1996-05-31
CA2153657A1 (en) 1994-07-21
FI930122A (en) 1994-07-13
EP0679255A1 (en) 1995-11-02

Similar Documents

Publication Publication Date Title
CA1304836C (en) Method for detection of alien matter contents in gases
US5032721A (en) Acid gas monitor based on ion mobility spectrometry
EP0509171B1 (en) Method and apparatus for improving the specificity of an ion mobility spectrometer utilizing sulfur dioxide dopant chemistry
EP0679886B1 (en) Ion mobility spectrometer
US7030372B2 (en) Micromachined field asymmetric ion mobility filter and detection system
US4724394A (en) Gas detection by ion mobility segregation
US3768302A (en) Method and apparatus for sensing substances by analysis of adsorbed matter associated with atmospheric particulates
CA2474561A1 (en) Faims apparatus and method for detecting trace amounts of a vapour in a carrier gas
US7244931B2 (en) Ion mobility spectrometer with parallel running drift gas and ion carrier gas flows
CN1361922A (en) Micromachined field asymmetric ion mobility filter and detection system
US5281915A (en) Sensor for detecting a high molecular weight substance using ionization effects
EP0679255A1 (en) Method and equipment for definition of foreign matter contents in gases
US6627878B1 (en) (Chemical agent) point detection system (IPDS) employing dual ion mobility spectrometers
US6987262B2 (en) FAIMS apparatus and method for detecting trace amounts of a vapour in a carrier gas
US7956323B2 (en) Ion mobility spectrometer and method for determining an analyte substance or an analyte substance mixture in the presence of a dopant mixture by means of an ion mobility spectrometer
CA2668477A1 (en) Faims ion mobility spectrometer with multiple doping
US3668382A (en) Separation and detection of trace substances in gaseous samples containing moisture by diluting with dry air
US4119851A (en) Apparatus and a method for detecting and measuring trace gases in air or other gas backgrounds
EP2076765A1 (en) Spectrometer apparatus
RU2277238C2 (en) Method of measurement of concentration of impurities in nitrogen, hydrogen and oxygen by means of ion mobility spectrometry
EP0457776B1 (en) Gas detector
RU2178929C2 (en) Spectrometer of non-linearity of drift of ions
Zimmermann et al. A miniaturized ion mobility spectrometer for detection of hazardous compounds in air
RU2289810C2 (en) Corona discharge ionization source for devices detecting microscopic impurities of matter in gases
SU1004873A1 (en) Ionization detector for gas chromatography

Legal Events

Date Code Title Description
AK Designated states

Kind code of ref document: A1

Designated state(s): CA JP NO RU US

AL Designated countries for regional patents

Kind code of ref document: A1

Designated state(s): AT BE CH DE DK ES FR GB GR IE IT LU MC NL PT SE

DFPE Request for preliminary examination filed prior to expiration of 19th month from priority date (pct application filed before 20040101)
121 Ep: the epo has been informed by wipo that ep was designated in this application
WWE Wipo information: entry into national phase

Ref document number: 2153657

Country of ref document: CA

WWE Wipo information: entry into national phase

Ref document number: 1994904196

Country of ref document: EP

ENP Entry into the national phase

Ref document number: 1995 481491

Country of ref document: US

Date of ref document: 19950901

Kind code of ref document: A

WWP Wipo information: published in national office

Ref document number: 1994904196

Country of ref document: EP

ENP Entry into the national phase

Ref document number: 1997 979277

Country of ref document: US

Date of ref document: 19971126

Kind code of ref document: A

WWW Wipo information: withdrawn in national office

Ref document number: 1994904196

Country of ref document: EP