Periodically alternating path and alternating wavelength bridges for quantitative and ultrasensitive measurement of vapor concentration

• US 5,381,010 A
• Filed: 12/03/1993
• Issued: 01/10/1995
• Est. Priority Date: 12/03/1993
• Status: Expired due to Fees

• Current Assignee: Sleepair Corporation
• Original Assignee: Sleepair Corporation
• Inventors: Gordon, Eugene I.
• Primary Examiner(s): Dzierzynski, Paul M.
• Assistant Examiner(s): Dunn, Drew A.
• Application Number:
  US08/162,443
• Time in Patent Office: 403 Days
• Field of Search: 250/343, 250/345, 250/350, 250/351, 250/339.13, 356/437
• US Class Current: 250/343
• CPC Class Codes: G01J 1/16 using electric radiation detectors G01J1/20 takes precedence
• CPC Class Codes: G01N 21/314 with comparison of measurements at specific and non-specific wavelengths dual wavelength spectrometry G01J3/427
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis
• CPC Class Codes: G01N 2201/0621 Supply

Abstract

An apparatus for ultrasensitive detection of low concentrations of constituents using a broad band LED source is described. The apparatus provides enhanced resolution by synchronously detecting an imbalance between two analog signals due to absorption in a measurement cell at a wavelength of interest. Elements are provided to balance the signals in the absence of absorption to provide a reference point for concentration calculations. In accordance with several embodiments of the present invention, a time alternating signal for synchronous detection is achieved by combining signals from each of two alternating paths, only one of which travels through the measurement cell and which may have absorption. If there is absorption in the measurement cell, then the signal created by combining the alternating paths will exhibit residual modulation at the path alternation rate. In accordance with another embodiment of the present invention, a time alternating signal is achieved by combining signals from each of two alternating ultranarrow wavelength channels, each of which travels through the measurement cell but only one of which is on an absorption line of a constituent believed to be in the measurement cell, into a single photosensitive device. If there is absorption in the measurement cell, then the signal from the photosensitive device formed by combining the alternating wavelength channels will exhibit residual modulation at the wavelength channel alternation rate.

Claims

1. An apparatus for measuring optical absorption by a constituent gas in a measurement cell, said apparatus comprising:

radiation means for emitting broad band infrared radiation along one of a measurement lightpath and a reference lightpath, the measurement cell being positioned in said measurement lightpath so that said radiation passes therethrough;

alternating means for alternately and periodically directing said radiation along one of said lightpaths at a first frequency;

attenuating means for balancing the relative power of said radiation in each of said lightpaths in the absence of optical absorption of the constituent in the measurement cell;

sensor means for sensing radiation from each of said lightpaths and for producing a sensed signal, said sensed signal exhibiting modulation thereupon at said first frequency only when there is optical absorption of the constituent in the measurement cell; and

synchronous detection means for demodulating said first frequency from said sensed signal so as to extract a DC signal, said DC signal being proportional to the optical absorption of the constituent in the measurement cell.

2. An apparatus as in claim 1 further including modulating means for modulating said emitted radiation at a second frequency so that said radiation in each of said alternating lightpaths is modulated, and demodulating means connected between said sensor means and said synchronous detection means for demodulating said second frequency from said sensed signal.

3. An apparatus as in claim 2 wherein said second frequency is higher than said first frequency and further chosen to be above a flicker noise region of said sensor means.

4. An apparatus as in claim 1 further comprising calibration or calculation means for relating said DC signal from said synchronous detection means to the concentration of the constituent in the measurement cell.

5. An apparatus as in claim 1 further comprising means for thermally tuning said radiation means so that said radiation means emits a band of radiation centered on an absorption line of the constituent in the measurement cell.

6. An apparatus as in claim 1 wherein said detected signal also exhibits residual modulation when there is an imbalance in the relative power from said radiation means traversing said lightpaths, and said DC signal is an indication of said imbalance in the absence of optical absorption of the constituent in the measurement cell.

7. An apparatus for measuring optical absorption by a constituent gas in a measurement cell, said apparatus comprising:

radiation means for emitting broad band infrared radiation along one of a measurement lightpath and a reference lightpath, the measurement cell being positioned in said measurement lightpath so that said radiation passes therethrough;

modulating means for modulating said emitted radiation at a first frequency;

alternating means for alternately and periodically directing said radiation along one of said lightpaths at a second frequency;

attenuating means for balancing the relative power of said radiation in each of said lightpaths in the absence of optical absorption of the constituent in the measurement cell;

sensor means for sensing radiation from each of said lightpaths and for producing a sensed signal;

demodulating means for demodulating said first frequency from said sensed signal and extracting a detected signal, said detected signal exhibiting a residual modulation thereupon at said second frequency only when there is optical absorption of the constituent in the measurement cell; and

synchronous detection means for demodulating said second frequency from said detected signal so as to extract a DC signal, said DC signal being proportional to the absorption by the constituent in the measurement cell.

8. An apparatus according to claim 7 further comprising filtering means positioned ahead of said sensor means for passing only an ultranarrow range of wavelengths from each of said lightpaths to said sensor means.

9. An apparatus as in claim 8 further comprising means for tuning said filtering means so that said filtering means passes an ultranarrow range of wavelengths centered on an absorption line of the constituent in the measurement cell.

10. An apparatus as in claim 7 wherein said alternating means comprises a light reflecting chopper and said attenuating means comprise parallel plates of optical material.

11. An apparatus as in claim 10 wherein said reflecting chopper alternately passes said radiation directly through one of said paths and to a first 90°

reflecting mirror and reflects said radiation in the other of said paths 90°

to a second 90°

reflecting mirror and from there to a third 90°

reflecting mirror so that said radiation from both of said paths travels in parallel toward said sensor means.

12. An apparatus as in claim 7 further comprising calibration or calculation means for relating said DC signal from said synchronous detection means to the concentration of the constituent in the measurement cell.

13. An apparatus as in claim 7 further comprising means for thermally tufting said radiation means so that said radiation means emits a band of radiation centered on an absorption line of the constituent in the measurement cell.

14. An apparatus as in claim 7 wherein said detected signal also exhibits residual modulation when there is an imbalance in the relative power of light from said radiation means traversing said lightpaths, and said DC signal is an indication of said imbalance in the absence of optical absorption of the constituent in the measurement cell.

15. An apparatus as in claim 7 wherein said first frequency is above 8 MHz and said second frequency is below 2000 Hz.

16. An apparatus as in claim 7 further comprising a selectively connectable logarithmic circuit between said demodulating means and said synchronous detection means.

17. An apparatus for measuring optical absorption by a constituent gas in a measurement cell, said apparatus comprising:

radiation means for emitting broad band infrared radiation along one of a measurement lightpath and a reference lightpath, the measurement cell being positioned in said measurement lightpath so that said radiation passes therethrough;

modulating means for modulating said emitted radiation at a first frequency;

alternating means for alternately and periodically directing said radiation along one of said lightpaths at a second frequency;

attenuating means for balancing the relative power of said radiation in each of said lightpaths in the absence of optical absorption of the constituent in the measurement cell;

first and second sensor means for sensing radiation from each of said lightpaths and for producing a pair of sensed signals;

filtering means positioned ahead of said first and second sensor means for passing only an ultranarrow range of wavelengths from each of said lightpaths to said first sensor means and reflecting the remainder of said radiation band to said second sensor means;

demodulating means for demodulating said first frequency from said pair of sensed signals and extracting a pair of detected signals, said pair of detected signals exhibiting a residual modulation thereupon at said second frequency only when there is optical absorption of the constituent in the measurement cell; and

synchronous detection means for demodulating said second frequency from each of said pair of detected signals so as to extract a pair of DC signals, the one of said DC signals from said first sensor means being proportional to the optical absorption of the constituent in the measurement cell and the other of said DC signals from said second sensor means being proportional to any broad band absorption in the measurement cell.

18. An apparatus as in claim 17 further comprising means for tuning said filtering means so that said filtering means passes an ultranarrow range of wavelengths centered on an absorption line of the constituent in the measurement cell.

19. An apparatus as in claim 18 further comprising means for thermally tuning said radiation means so that said radiation means emits a band of radiation centered on an absorption line of the constituent in the measurement cell.

20. An apparatus as in claim 17 further comprising calibration or calculation means for relating said DC signal of said synchronous detection means to the concentration of the constituent in the measurement cell.

21. An apparatus as in claim 17 wherein said pair of detected signals also exhibit residual modulation when there is an imbalance in the relative power of light traversing said lightpaths and either of said pair of DC signals is an indication of said imbalance in the absence of optical absorption of the constituent in the measurement cell.

22. An apparatus for measuring optical absorption by a constituent gas in a measurement cell, said apparatus comprising:

radiation means for emitting broad band infrared radiation along a measurement lightpath, the measurement cell being positioned in said lightpath so that said radiation passes therethrough;

modulating means for modulating said emitted radiation at a predetermined frequency;

filtering means positioned behind the measurement cell for optically splitting said radiation into an absorption channel and a reference channel, said absorption channel having only an ultranarrow range of wavelengths from said lightpath, said reference channel having the remainder of said radiation band;

a first sensor means for sensing radiation in said absorption channel and for producing a first sensed signal;

a second sensor means for sensing radiation in said reference channel and producing a second sensed signal;

attenuating means disposed in one of said absorption and reference channels for balancing the relative power of light therein in the absence of optical absorption of the constituent in the measurement cell;

demodulating means for demodulating said predetermined frequency from each of said first and second sensed signals and extracting a respective pair of detected signals;

analog-to-digital convertor means for converting said pair of detected signals to a respective pair of digital detected signals; and

a digital differential amplifier having a pair of differential inputs connected to said pair of digital detected signals and having an output proportional to the optical absorption of the constituent in the measurement cell.

23. An apparatus as in claim 22 further comprising means for tuning said filtering means so that said filtering means passes an ultranarrow range of wavelengths centered on an absorption line of the constituent in the measurement cell.

24. An apparatus as in claim 23 further comprising means for thermally tuning said radiation means so that said radiation means emits a band of radiation centered on an absorption line of the constituent in the measurement cell.

25. An apparatus as in claim 22 further comprising calibration or calculation means for relating said DC signal of said synchronous detection means to the concentration of the constituent in the measurement cell.

26. An apparatus as in claim 22 further comprising digital signal processing means connected between said analog-to-digital convertors and said digital differential amplifier.

27. An apparatus as in claim 22 wherein said predetermined frequency is above 8 MHz.

28. An apparatus as in claim 22 wherein said attenuating means comprise parallel plates of optical material.

29. An apparatus as in claim 22 wherein said first and second sensor means operate continuously and contemporaneously so that said digital differential amplifier provides a continuous concentration measurement.

30. An apparatus for measuring optical absorption by a constituent gas in a measurement cell, said apparatus comprising:

radiation means for emitting broad band infrared radiation along a measurement lightpath, the measurement cell being positioned in said lightpath so that said radiation passes therethrough;

sensor means for sensing radiation from said lightpath and for producing a sensed signal;

filtering means positioned ahead of said sensor means for passing only an ultranarrow range of wavelengths, the relative angle of said filtering means with respect to said lightpath influencing which ultranarrow range of wavelengths is passed by said filtering means;

vacillating means for alternately and periodically positioning said filtering means at an angle of one of θ and

θ

±

Δ

θ

degrees with respect to said lightpath, said vacillating means vacillating at one predetermined frequency;

said filtering means passing wavelengths centered on λ

_A when said filtering means is positioned at θ

degrees and passing wavelengths centered on λ

_B when said filtering means is positioned at θ

±

Δ

θ

degrees, Δ

θ

being chosen so that only one of λ

_A and λ

_B is centered on an optical absorption line of the constituent in the measurement cell; and

synchronous detection means for demodulating said one predetermined frequency from said sensed signal so as to extract a DC signal, said DC signal being proportional to the optical absorption of the constituent in the measurement cell.

31. An apparatus according to claim 30 wherein said DC signal is proportional to the optical absorption power differential between λ

_A and λ

_B.

32. An apparatus according to claim 30 wherein said vacillating means is a cam, said cam having one surface for positioning said filtering means at an angle θ

with respect to said lightpath and another surface for positioning said filtering means at an angle θ

±

Δ

θ

with respect to said lightpath.

33. An apparatus as in claim 30 further comprising means for thermally tuning said radiation means so that said radiation means emits equal energy at each of λ

_A and λ

_B and so that said DC signal from said synchronous detection means is zero in the absence of optical absorption of the constituent in the measurement cell.

34. An apparatus as in claim 30 further comprising means for tuning said filtering means so that said filtering means passes an ultranarrow range of wavelengths centered on an absorption line of the constituent in the measurement cell.

35. An apparatus according to claim 30 further comprising modulating means for modulating said emitted radiation at another predetermined frequency and demodulating means connected between said sensor means and said synchronous detection means for demodulating said another predetermined frequency from said sensed signal.

36. An apparatus as in claim 30 further comprising calibration or calculation means for relating said DC signal of said synchronous detection means to the concentration of the constituent in the measurement cell.