Method and apparatus for remote optical detection of a gas present in an observed volume

• US 5,306,913 A
• Filed: 12/03/1992
• Issued: 04/26/1994
• Est. Priority Date: 12/04/1991
• Status: Expired due to Term

• Current Assignee: Bertin & CIE
• Original Assignee: Bertin & CIE
• Inventors: Pelous, Gerard, Noack, Jean-Claude, Guern, Yves
• Primary Examiner(s): Hannaher, Constantine
• Application Number:
  US07/985,640
• Time in Patent Office: 509 Days
• Field of Search: 250/338.5, 250/330
• US Class Current: 250/338.5
• CPC Class Codes: G01M 3/38 by using light G01M3/02 takes precedence
• CPC Class Codes: G01N 2021/177 Detector of the video camera type
• CPC Class Codes: G01N 2021/1793 Remote sensing
• CPC Class Codes: G01N 2021/3129 Determining multicomponents by multiwavelength light
• CPC Class Codes: G01N 2021/3181 using LEDs
• CPC Class Codes: G01N 2021/3531 without instrumental source, i.e. radiometric
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis

Abstract

A method and apparatus for remote optical detection of a gas present in an observed volume using a thermal imager or camera including one or more sensitive elements which are sensitive to radiant fluxes in a determined band of wavelengths, two filters interposable on the optical axis of the camera, the filters having similar transmission bands, one of which includes an absorption line characteristic of the looked-for gas, while the other of which is complementary to said absorption line, and signal processing means for taking the difference between the radiated fluxes received from two points at different temperatures in the volume as observed first through one of the filters and then through the other filter, for taking the ratio of said differences, and for deducing therefrom whether the gas is present in the observed volume.

Claims

1. A method for remote optical detection of a gas, e.g. a polluting gas, present in an observed volume, the method comprising:

detecting the radiant fluxes coming from at least two different temperature points of said volume, said fluxes passing through the looked-for gas and being detected through a first filter having a transmission band that includes an absorption line characteristic of the looked-for gas;

taking the difference between the fluxes detected through the first filter;

detecting the radiant fluxes coming from the above-specified two points through a second filter having a transmission band similar to that of the first filter and complementary to said absorption line of the looked-for gas;

taking the difference between the fluxes detected through the second filter;

taking the ratio of the above-specified differences; and

deducing possible presence of the gas in the observed volume from the value of said ratio.

2. A method according to claim 1, further comprising detecting the above-mentioned fluxes through one of the filters F1, and then through both filters F1, F2 while they are superposed.

3. A method according to claim 1, further comprising using a thermal imager or camera for detecting the above-mentioned fluxes, and processing the electrical signals provided by the thermal imager or camera in the above-mentioned manner, which signals correspond to the above-mentioned fluxes.

4. A method according to claim 3, further comprising:

digitizing the signals provided by the thermal imager or camera;

applying the digitized signals to a data processing center; and

using said system to obtain time averages and local or geographic averages on said signals by integration in order to reduce noise and increase measurement accuracy.

5. A method according to claim 1, further comprising:

detecting fluxes from areas that are distributed in predetermined manner within the observed volume through one filter and then through the other filter;

comparing the flux from an area with the fluxes from adjacent areas to obtain first differences between the fluxes detected through one of the filters and second differences between the fluxes detected through the other filter and deducing a map of gas concentration in the observed volume from the ratios between the first differences and the second differences.

6. A method according to claim 1, in which, in order to detect two different gases in the observed volume, the method comprises using two filters having similar transmission bands, the band of one of the filters being complementary to an absorption line characteristic of one of the two gases, and the band of the other filter being complementary to an absorption line characteristic of the other one of the gases, the method further comprising deducing the presence of one or other of the gases in the observed volume from the value of the ratio of the fluxes detected through each of the two filters.

7. A method according to claim 1, in which, in order to detect two different gases in the observed volume, the method further comprising using two filters having similar transmission bands, the band of one of the filters including an absorption line characteristic of one of the two gases and another absorption line characteristic of the other gas, the transmission band of the other filter being complementary to said absorption lines, and in deducing in presence of one or other of the gases in the observed volume on the basis of the value of the ratio of the fluxes detected through each of the two filters.

8. Apparatus for remote optical detection of a gas, in an observed volume, e.g. a polluting gas, the apparatus comprising:

a thermal imager or camera including at least one sensitive element sensitive to radiant fluxes in a determined band of wavelengths, and an optical system enabling an image of at least a portion of the observed volume to be formed on said sensitive element;

at least two filters suitable for being interposed on the optical axis of the thermal imager or camera for detecting the radiant fluxes of the observed volume through each of the filters, said filters having similar transmission bands in the above-mentioned band of wavelengths, the band of one of the filters including at least one absorption line of the lookedfor gas and the band of the other filter being complementary to said absorption line; and

signal processing means comprising means for selecting the signals provided by said sensitive element and corresponding to the fluxes from at least two points at different temperatures in the observed volume, the fluxes from these two points being detected through the looked-for gas, means for establishing the differences between the fluxes from these two points as detected through one and then the other one of the filters and means for taking the ratio of these differences.

9. Apparatus according to claim 8, comprising means for comparing fluxes from adjacent areas in the observed volume, for obtaining the differences between said fluxes as detected through one of the filters and the differences between these fluxes as detected through the other filter, means for establishing the ratios between said differences, and means for comparing said ratios to establish a map of the concentration of the gas in the observed volume.

10. Apparatus according to claim 8, comprising means for digitizing the signals provided by the sensitive element.

11. Apparatus according to claim 8, in which, to detect a second gas present in the observed volume and characterized by another absorption line in the above-mentioned band of wavelengths, the transmission bands of the two above-mentioned filters are respectively complementary to the absorption line of the first line and to the absorption line of the second gas.

12. Apparatus according to claim 8, in which, to detect other gases present in the observed volume and characterized by other absorption lines in the above-specified band of wavelengths, the transmission bands of the two above-mentioned filters are determined so that one of them includes the absorption lines of the looked-for gases while the other one is complementary to said absorption lines.

13. Apparatus according to claim 8, in which the transmission bands of the above-mentioned filters are of widths in wavelength that are so determined that the fluxes received by the thermal imager or camera correspond to a linear response region of the thermal imager or camera.