Gas Sensor Based On Photoacoustic Detection

• US 20110072886A1
• Filed: 09/30/2009
• Published: 03/31/2011
• Est. Priority Date: 09/30/2009
• Status: Abandoned Application

• Current Assignee: Corning Incorporated
• Original Assignee: Corning Incorporated
• Inventors: Xie, Feng, Pollard, Scott Christopher, Liu, Anping, Caneau, Catherine Genevieve, Zah, Chung-En
• Application Number:
  US12/570,606
• Publication Number:
  US 20110072886A1
• Time in Patent Office: Days
• US Class Current: 73/24.02
• CPC Class Codes: G01N 2021/1704 in gases
• CPC Class Codes: G01N 21/1702 with opto-acoustic detection, e.g. for gases or analysing solids

Abstract

A photoacoustic gas detector and photoacoustic gas detection method are disclosed. The detector includes a laser source, an acoustic resonator, and at least one tuning fork positioned along a longitudinal length of the resonator. The detector is capable of performing fast measurements of the concentration of one or more target gases over a broad temperature range.

Claims

1. A photoacoustic gas detector for detecting the concentration of at least one target gas, the gas detector comprising:

a laser source;

a resonator extending along a longitudinal axis, the resonator having a first end, a second end, and an inner cavity between the first end and the second end, the inner cavity extending along the longitudinal axis and defining a longitudinal opening between the first end and the second end, the inner cavity adapted to allow a laser beam from the laser source to pass through the longitudinal opening; and

at least one tuning fork positioned along a longitudinal length of the resonator, said tuning fork comprising a first prong and a second prong, wherein the longitudinal axis does not intersect an area between the first prong and the second prong.

2. The gas detector of claim 1, wherein the resonator comprises a cylindrical tube.

3. The gas detector of claim 1, wherein the first prong and the second prong are generally parallel to the longitudinal axis.

4. The gas detector of claim 1, wherein the first prong and the second prong are generally perpendicular to the longitudinal axis.

5. The gas detector of claim 1, wherein the gas detector is capable of detecting at least one target gas at a concentration of less than 200 parts per million.

6. The gas detector of claim 1, wherein the resonator has a structural resonance frequency that substantially coincides with a structural resonance frequency of the tuning fork.

7. The gas detector of claim 1, wherein said resonator and said tuning fork are integrated on a single platform.

8. The gas detector of claim 1, wherein said resonator has a parabolic cross section and the tuning fork is at least partially positioned on a focal point of the parabolic cross section.

9. The detector of claim 1, wherein the detector is capable of detecting the concentration of at least two target gases.

10. The detector of claim 1, wherein the at least one tuning fork comprises at least two tuning forks.

11. A method for determining the concentration of at least one target gas using photoacoustic detection, the method comprising:

directing a laser beam from a laser source into an inner cavity of an acoustic resonator, the resonator and the inner cavity extending along a longitudinal axis, the inner cavity containing a concentration of the at least one target gas, wherein interaction between the laser beam and the at least one target gas causes accumulation of an acoustic signal in the resonator;

generating a resonant absorption signal relative to the concentration of the at least one target gas by at least one tuning fork positioned along a longitudinal length of the resonator, said tuning fork comprising a first prong and a second prong, wherein the longitudinal axis does not intersect an area between the first prong and the second prong.

12. The method of claim 11, wherein the resonator comprises a cylindrical tube.

13. The method of claim 11, wherein the method is capable of detecting at least one target gas at a concentration of less than 200 parts per million.

14. The method of claim 11, wherein the resonator has a structural resonance frequency that substantially coincides with a structural resonance frequency of the tuning fork.

15. The method of claim 11, wherein the resonant absorption signal is at least 10 times greater than a background noise signal.

16. The method of claim 11, wherein the at least one tuning fork comprises at least two tuning forks.

17. The method of claim 16, wherein the method is capable of generating a resonant absorption signal relative to the concentration of the at least one target gas while calibrating for the temperature and pressure in the inner cavity of the resonator.

18. The method of claim 11, wherein the method is capable of generating a resonant absorption signal relative to the concentration of the at least one target gas within one second of first directing the laser beam from the laser source into the inner cavity of the resonator.

19. The method of claim 11, wherein the method is capable of generating a resonant absorption signal relative to the concentration of the at least one target gas at a temperature of at least 700°

C.

20. The method of claim 11, wherein the laser source produces at least one emission wavelength with a spectral linewidth narrower than the absorption bandwidth of the gas.

21. The method of claim 11, wherein the laser source is capable of tuning its wavelength to find the absorption peak of the at least one target gas.