Method and device for detection and identification of gases

• US 9,404,889 B2
• Filed: 01/12/2009
• Issued: 08/02/2016
• Est. Priority Date: 01/19/2008
• Status: Active Grant

• Current Assignee: Airsense Analytics GmbH
• Original Assignee: Airsense Analytics GmbH
• Inventors: Mnchmeyer, Wolf, Ungethm, Bert, Walte, Andreas
• Primary Examiner(s): LOGIE, MICHAEL J
• Application Number:
  US12/863,553
• Publication Number:
  US 20100314548A1
• Time in Patent Office: 2,759 Days
• Field of Search: 250281-300
• US Class Current: 1/1
• CPC Class Codes: G01N 27/622 Ion mobility spectrometry
• CPC Class Codes: G01N 27/624 Differential mobility spectrometry [DMS]; Field asymmetric-waveform ion mobility spectrometry [FAIMS]
• CPC Class Codes: H01J 49/0027 Methods for using particle spectrometers
• CPC Class Codes: H01J 49/0031 Step by step routines describing the use of the apparatus H01J49/0081 takes precedence

Abstract

Methods and devices identify gases and allow immediate and simultaneous detection of the chemical compounds to be tested. The methods and devices use a function of the electric field strength, for identification the material-specific mobility and simultaneously the change in this mobility, which is achieved in that due to the resulting electric field, each ionized molecule has a drift velocity which is partially increased or decreased, wherein the resulting electric field is a DC field, on which an asymmetric AC field is superimposed. The methods and devices for the detection and identification of gases are used to identify and detect chemical compounds, such as, explosive and/or unhealthy substances or compounds, which may be detected in very small concentrations.

Claims

1. A device for identification of gases, comprising an inlet system and at least one detector, wherein at least one drift tube is delimited, on one hand, by the inlet system and, on the other hand, by the at least one detector, and that in each drift tube an opening and closing grid is disposed which divides an interior space of the drift tube into a reaction space and a drift space, wherein an ion source is arranged in the reaction space and a shield grid is arranged in the drift space, wherein the drift tube comprises several DC voltage electrodes, arranged around and along the reaction space and the drift space, that produce a constant electric field in the reaction space and the drift space, and AC voltage electrodes, wherein the AC voltage electrodes are distributed regionally along the length of the drift space, wherein the AC voltage electrodes of the drift tube comprise at least three AC voltage electrodes in the drift space, that produce an alternating asymmetric electric field in a region of the drift space operating along the same coordinate axis as the constant electric field, and the DC voltage electrodes and the AC voltage electrodes are arranged around the drift space, that each ionized molecule in the region of the drift space has a drift velocity caused by a resulting electric field, wherein the resulting electric field is the constant DC voltage field, on which the asymmetric AC voltage field is locally superimposed, wherein change in the drift velocity is due to each ionized molecule performing, due to the resulting electric field, a constant drift movement on which an oscillatory movement is superimposed, so that the ionized molecule performs a drift movement in one direction, that runs parallel to field lines of the resulting electric field, with the oscillatory movement superimposed collinear thereto.

2. The device according to claim 1, wherein an additional drift tube is delimited, on one hand, by the inlet system and, on the other hand, by an additional detector, wherein the drift tubes have opposite polarities.

3. The device according to claim 1, wherein the drift tube comprises alternatingly arranged metal rings and isolator rings, wherein each metal ring is electrically connected around the drift space and forms a respective DC voltage electrode.

4. The device according to claim 1, wherein the drift tube comprises one or more tubes with low electric conductivity.

5. The device according to claim 1, wherein the AC voltage electrodes comprise thin wire grids extending transversely through the drift space.

6. The device according to claim 1, wherein the opening and closing grid comprises two electrically conducting metal combs, which are arranged in a plane extending transversely through the drift tube, wherein the metal combs are slightly offset from one another and do not contact each other.

7. The device according to claim 6, wherein the opening and closing grid has two switching states, wherein:

in a first switching state, the opening and closing grid is closed, because the metal combs are at different potentials and this potential difference produces a high field strength, thereby preventing ions from passing through the opening and closing grid, and

in a second switching state, the opening and closing grid is open, because the metal combs are at the same potential, so that no electric field at all or only an electric field with a low field strength is produced, allowing ions to pass through the opening and closing grid.

8. The device according to claim 1, wherein the shield grid is arranged in front of the detector, wherein the shield grid provides capacitive decoupling.

9. The device according to claim 1, wherein the drift tube comprises at least one auxiliary electrode which is arranged in the drift space for generating an additional compensation voltage.

10. The device according to claim 1, wherein the drift tube is constructed as a circular cylinder.

11. A method for identification of gases, wherein the gases to be identified are ionized and drift times of the ionized molecules through a drift space are measured and the measured drift times are evaluated by a gas identification device comprising at least one drift tube an inlet system and at least one detector, wherein the at least one drift tube is delimited, at a first end end, by the inlet system and, at a second end, by the at least one detector, wherein an opening and closing grid is disposed within the at least one drift tube and divides an interior of the drift tube into a reaction space and the drift space, wherein the drift tube comprises several DC voltage electrodes, arranged around and along the reaction space and drift space, that produce a constant electric field in the reaction space and drift space, and AC voltage electrodes, wherein the AC voltage electrodes are distributed regionally along the length of the drift space, that produce an alternating asymmetric electric field in a region of the drift space operating along the same coordinate axis as the constant electric field, wherein the DC voltage electrodes and the AC voltage electrodes are arranged around the drift space, wherein, for measurement of the drift times, the ionized molecules are firstly accelerated to a drift velocity in the drift space by the constant electric field and secondly ionized molecules that have the same drift velocity commonly enter the region in the drift space, wherein a resulting electric field formed by the constant electric field, on which the alternating asymmetric electric field is locally superimposed, additionally accelerates or decelerates the ionized molecules so that each ionized molecule has a drift velocity caused by the resulting electric field, wherein change in the drift velocity is due to each ionized molecule performing, due to the resulting electric field, a constant drift movement on which an oscillatory movement is superimposed, so that the ionized molecules perform a drift movement in one direction, that runs parallel to field lines of the resulting electric field, with the oscillatory movement superimposed collinear thereto.

12. The method according to claim 11, wherein positive and/or negative ions are used as ionized molecules.

13. The method according to claim 11, wherein each ionized molecule is accelerated and decelerated several times, wherein on average, depending on the material properties of the molecule, the acceleration is greater or smaller than the deceleration.

14. The method according to claim 11, wherein the DC voltage field has a low electric field strength, and the asymmetric AC voltage field has a high electric field strength.

15. The method according to claim 14, wherein an amplitude of asymmetric AC voltage is changed during the measurement of the drift times.

16. The method according to claim 11, wherein, for identification of the chemical compounds, the measured drift times are compared with previously determined drift times of known chemical compounds.

17. The method according to claim 16, wherein the comparison between the measured drift times and the known drift times of chemical compounds is performed using mathematical or statistical methods.

18. The method according to claim 11, wherein the drift times of ionized molecules having identical mobilities at low electric field strengths are compared with the drift times of these ionized molecules after the asymmetric AC voltage field with a high electric field strength generated by the AC voltage electrodes is switched in, and that for identification of the chemical compounds, the measured drift times are compared with the previously determined drift times.