Correction of collision broadening in non-dispersive absorption measurement of gases

• US 5,900,635 A
• Filed: 10/18/1995
• Issued: 05/04/1999
• Est. Priority Date: 09/29/1995
• Status: Expired due to Term

• Current Assignee: Instrumentarium Dental Incorporated (Envista Holdings Corporation)
• Original Assignee: Instrumentarium Corporation
• Inventors: Weckstrom, Kurt Peter
• Primary Examiner(s): Hannaher, Constantine
• Application Number:
  US08/544,663
• Time in Patent Office: 1,294 Days
• Field of Search: 250/345, 250/343, 128/719, 356/437, 600/532
• US Class Current: 250/345
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis

Abstract

A method of non-dispersive analysis of gas mixtures for determining the concentration of some gas component therein. A radiation source is arranged which emits, through the gas mixture being analyzed, radiation within a wavelength range within which the absorption spectrum band used in the determination of the concentration of the said gas component is located; an optical transmission band filter the transmission band of which coincides with the said spectrum band is provided in the path of the radiation traversing the gas mixture being analyzed; a detector is used for detecting the radiation which has traversed the gas mixture being analyzed and the optical transmission band filter, whereby a first signal is obtained from the detector; a different second signal is generated in the detector by means of an additional gas or an additional gas mixture interposed between the radiation source and the detector; and the result of the concentration measurement is formed computationally by using the different measurement signals. Furthermore, in the method the transmission bands of the said transmission band filters are arranged within the same measuring range; as the additional gas there is used a compensation gas or a compensation gas mixture in which the compensation gas is the gas component the concentration of which is being determined or a corresponding other gas or a compensation filter. The absorption properties of the compensation filter are selected to be such, or the amount of the compensation gas is selected to be such, that the broadening of the absorption lines in the absorption spectrum band used will change the said different second signal.

Claims

1. A method for determining the concentration of a given gas in a mixture of gases by means of non-dispersive absorption of radiation, the method providing compensation for the effects of collision broadening of absorption lines in the absorption spectrum of the given gas, said method comprising the steps of:

(a) providing a sample of the gas mixture;

(b) passing radiation through the gas mixture, the radiation having a wavelength range including an absorption spectrum band for determining the concentration of the given gas;

(c) applying the radiation exiting the gas mixture to a first optical transmission band filter, the first filter having a transmission bandwidth selected from a range of bandwidth values having a maximum value substantially equal to the width of the absorption spectrum band and a minimum value less than the width of the absorption spectrum band;

(d) detecting the intensity of the radiation transmitted through the first optical transmission band filter to provide a first signal, the detected radiation, and hence the first signal, being subject to the effects of collision broadening occurring from the mixture of gases;

(e) providing a compensation filter, the compensation filter including a compensating gas including a known concentration of the given gas at a known pressure, any collision broadening effects occurring in the compensating gas usually differing from those occurring in the gas mixture;

(f) passing radiation through both the gas mixture and the compensating gas;

(g) applying the radiation passed through the gas mixture and compensating gas to a second optical transmission band filter, the second filter having a transmission bandwidth selected from a range of bandwidth values having a maximum value greater than the width of the absorption spectrum band and a minimum value less than the width of the absorption spectrum band;

(h) detecting the intensity of the radiation transmitted through the second filter to provide a second signal, the detected radiation, and hence the second signal, being subject to the differing collision broadening effects resulting from passage through the compensating gas; and

(i) providing an output from the first and second signals which is compensated for the effects of collision broadening in the absorption spectrum of the given gas and is, thus, an accurate determination of the concentration of the given gas in the gas mixture.

2. A method according to claim 1 wherein step (e) is further defined as providing a compensation filter with a compensating gas in which the absorption lines of the given gas are not substantially broadened and wherein the amount of compensating gas included in the compensation filter is such that the intensity of the radiation detected and second signal provided in step (h) decrease as the collision broadening of the absorption lines of the given gas in the gas mixture increases.

3. A method according to claim 1 wherein step (e) is further defined as providing a compensation filter in which the amount of compensating gas is such that the intensity of the radiation detected in step (h), when the gas mixture contains a mean expected concentration of the given gas, is in a range of 0.01% and to 50% of the radiation intensity detected at step (d) when no substantial broadening of the absorption lines of the given gas occurs in the gas mixture.

4. A method according to claim 1 wherein step (c) is further defined as applying the radiation to a first optical transmission band filter having a transmission bandwidth which is substantially equal to the width of the absorption spectrum band.

5. A method according to claim 1 wherein step (c) is further defined as applying the radiation to a first optical transmission band filter having a transmission bandwidth which is narrower than the width of the absorption spectrum band but substantially wider than the width of an absorption line.

6. A method according to claim 1 wherein step (c) and (g) are further defined as applying radiation to optical transmission band filters having the same transmission bandwidth.

7. A method according to claim 1 wherein steps (b) and (f) are further defined as passing radiation from a single radiation source and wherein the detecting in steps (d) and (h) are carried out simultaneously.

8. A method according to claim 1 wherein radiation passing steps (b) and (f) are further defined as being carried out on an alternating basis and wherein steps (d) and (h) are carried out to alternately provide signals.

9. A method according to claim 8 wherein steps (d) and (h) are carried out using a single detector.

10. A method according to claim 1 wherein steps (b) and (f) are further defined as passing radiation from a single radiation source, wherein steps (d) and (h) are carried out using a single detector, and wherein step (e) is further defined as providing and removing the compensation filter from a radiation path extending between the radiation source and the detector, the provision of signals in steps (d) and (h) occurring successively.

11. A method according to claim 1 further including the steps of amplifying the first and second signals by different amplification coefficients and wherein step (i) is further defined as using the difference between said first and second signals to provide the compensated output.

12. A method according to claim 1 further defined as a method for determining the concentration of a given gas comprising carbon dioxide in a gas mixture comprising the respiration air of a subject.

13. A method according to claim 12 further defined as a method for determining the concentration of carbon dioxide in a gas mixture comprising the alveolar exhalation air of the subject.

14. An apparatus for providing an indication of the concentration of a given gas in a mixture of gases, said apparatus employing non-dispersive absorption of radiation and providing an output compensated for the effects of collision broadening of absorption lines in the absorption spectrum of the given gas, said apparatus comprising:

a sample chamber containing the gas mixture;

a radiation source means providing radiation to first and second radiation paths in said apparatus, the radiation having a wavelength range including an absorption spectrum band for determining the concentration of the given gas, said sample chamber being located in said first and second paths so that radiation from said radiation source means passes through said sample chamber;

a first optical transmission band filter located in said first radiation path for receiving radiation passed through said sample chamber, said first filter having a transmission bandwidth selected from a range of bandwidth values having a maximum value substantially equal to the width of the absorption spectrum band and a minimum value less than the width of the absorption spectrum band;

a compensation filter means located in said second radiation path, the compensation filter means including a compensating gas including a known concentration of the given gas at a known pressure, any collision broadening effects occurring in the compensating gas as usually differing from those occurring in the gas mixture;

a second optical transmission band filter in said second radiation path for receiving the radiation passed through said sample chamber and compensation filter means, said second filter having a transmission bandwidth selected from a range of bandwidth values having a maximum value substantially equal to the width of the absorption spectrum band and a minimum value less than the width of the absorption spectrum band;

detector means for detecting the intensity of the radiation transmitted through said first filter to provide a first signal, the detected radiation, and hence the first signal, being subject to the effects of collision broadening occurring from the mixture of gases, said detector means further detecting the intensity of the radiation transmitted through said second filter to provide a second signal, the detected radiation, and hence the second signal, being subject to the differing collision broadening effects resulting from passage through the compensating gas; and

means for applying the second signal to the first signal to provide an output which is compensated for the effects of collision broadening in the absorption spectrum of the given gas and is, thus, an accurate indication of the concentration of the given gas in the gas mixture.

15. An apparatus according to claim 14 wherein said compensation filter includes a compensating gas in which the absorption lines of the given gas are not substantially broadened and wherein the amount of compensating gas included in the compensation filter is such as to cause the intensity of the radiation detected and second signal provided by said detector means to decrease as the collision broadening of the absorption lines of the given gas in the gas mixture increases.

16. An apparatus according to claim 14 wherein said compensation filter includes an amount of compensating gas such that the intensity of the radiation detected by said detector means, when the gas mixture contains a mean expected concentration of the given gas, is in a range of 0.01% to 50% of the radiation intensity detected by said detector means when no substantial broadening of the absorption lines of the given gas occurs in the gas mixture.

17. An apparatus according to claim 14 wherein said first filter is further defined as having a transmission bandwidth which is substantially equal to the width of the absorption spectrum band.

18. An apparatus according to claim 14 wherein said first filter is further defined as having a transmission bandwidth which is narrower than the width of the absorption spectrum band but substantially wider than the width of an absorption line.

19. An apparatus according to claim 14 wherein said first and second filters have the same transmission bandwidth.

20. An apparatus according to claim 14 wherein said first and second filters comprise a single filter means.

21. An apparatus according to claim 14 wherein said radiation source means comprises a single radiation source.

22. An apparatus according to claim 14 wherein said radiation source means comprises a pair of radiation sources one of which provides radiation to said first radiation path, the other of which provides radiation to said second radiation path.

23. An apparatus according to claim 22 wherein said detector means comprises a first detector for said first radiation path and a second detector for said second radiation path.

24. An apparatus according to claim 14 wherein said first and second radiation paths are combined into a common radiation path extending from said radiation source means to said detector means, and wherein said compensation filter means is further defined as movable into and out of said common radiation path for providing said first and second signals from said detector means.

25. An apparatus according to claim 14 further including means for amplifying said first and second signals by different amplification coefficients and said applying means is further defined as using the difference between sand first and second signals to provide the compensated output.

26. An apparatus according to claim 14 further defined as an apparatus for providing an indication of the concentration of a given gas comprising carbon dioxide in a gas mixture comprising the respiration air of a subject.

27. An apparatus according to claim 26 further defined as an apparatus for providing an indication of the concentration of carbon dioxide in a gas mixture comprising the alveolar exhalation air of the subject.