Measuring low levels of methane in carbon dioxide

• US 20070259440A1
• Filed: 04/19/2007
• Published: 11/08/2007
• Est. Priority Date: 04/19/2006
• Status: Abandoned Application

• Current Assignee: Spectrasensors, Inc. (Endress+Hauser AG)
• Original Assignee: Spectrasensors, Inc. (Endress+Hauser AG)
• Inventors: Zhou, Xin, Sanger, Greg
• Application Number:
  US11/788,757
• Publication Number:
  US 20070259440A1
• Time in Patent Office: Days
• US Class Current: 436/141
• CPC Class Codes: G01N 21/05 Flow-through cuvettes G01N21/09 takes precedence; handling fluid samples G01N1/10
• CPC Class Codes: G01N 21/3504 for analysing gases, e.g. multi-gas analysis
• CPC Class Codes: G01N 21/39 using tunable lasers
• CPC Class Codes: G01N 33/004 for CO, CO2
• CPC Class Codes: G01N 33/0047 for organic compounds
• CPC Class Codes: Y02A 50/20 Air quality improvement or preservation, e.g. vehicle emission control or emission reduction by using catalytic converters
• CPC Class Codes: Y10T 436/214 Acyclic [e.g., methane, octane, isoparaffin, etc.]

Abstract

Low concentrations of methane in a gas mixture containing a substantial concentration of carbon dioxide can be detected and quantified using absorption spectroscopy in the infrared spectral region. Absorption spectra can recorded using tunable diode lasers as the light source. Modulation of the laser signal and demodulation of the resultant detector response yields dependable measurements that may be conducted with very little maintenance in demanding environments.

Claims

1. A method of detecting trace amounts of methane in carbon dioxide backgrounds, comprising:

directing a beam of light at a selected wavelength through a gas mixture comprising carbon dioxide and methane, the selected wavelength coinciding with a methane absorption feature that is resolvable from an absorption background due to carbon dioxide;

quantifying an absorption at the selected wavelength in the gas mixture; and

determining a methane concentration in the gas mixture based on the quantified absorption.

2. A method as in claim 1, wherein the gas mixture is contained within a sample cell that provides the path length.

3. A method as in claim 1, wherein the absorption at the selected wavelength is quantified with a photodetector that provides a detector output signal to a microprocessor.

4. A method as in claim 2, further comprising:

generating light with a range of wavelengths, the range of wavelengths comprising the selected wavelength;

tuning the generated light across the range of wavelengths; and

converting a DC signal from a photodetector that the light beam impinges upon after traversing the gas mixture to a second harmonic signal by demodulating the DC signal; and

analyzing the second harmonic signal to determine the methane concentration.

5. A method as in claim 1, wherein the methane concentration is less than or equal to approximately 50 ppm and the selected wavelength is in the range of about 1685 nm to 1700 nm.

6. A method as in claim 1, wherein the methane concentration is less than or equal to approximately 50 ppm and the selected wavelength is one of approximately 1654 nm, approximately 1687 nm, approximately 1694 nm, and approximately 1697 nm.

7. A method as in claim 1, wherein the methane concentration is in the range of approximately 1% to approximately 5% and the selected wavelength is in the range of about 1630 nm to 1660 nm.

8. A method as in claim 1, wherein the methane concentration is in a range of approximately 1% to 5%, and the selected wavelength is one of approximately 1637.4 nm, 1640.4 nm, 1642.9 nm, 1645.5 nm, 1648.2 nm, 1650.9 nm, 1653.7 nm, and 1656.5 nm.

9. A method as in claim 1, further comprising providing the beam of light from a tunable diode laser than is tuned to provide a range of wavelengths comprising the selected wavelength.

10. A method as in claim 1, further comprising maintaining the gas mixture and the photodetector at a constant temperature within a tolerance of approximately ±

1°

C.

11. An apparatus comprising:

a laser light source that emits at a selected wavelength that coincides with a methane absorption feature that is resolvable from an absorption background due to carbon dioxide;

a sample cell to contain a gas mixture containing methane and carbon dioxide with a methane concentration of less than or equal to approximately 5%, the sample cell providing a path length through the gas mixture of less than or equal to approximately 50 cm;

a photodetector positioned to quantify an intensity of light traversing the path length and to output a direct current data signal based on the quantified intensity; and

a microprocessor configured to receive and interpret the direct current signal from the photodetector and to determine the methane concentration in the gas mixture based on the direct current data signal and a calibration function.

12. An apparatus as in claim 11, wherein the methane concentration is less than or equal to approximately 50 ppm and the selected wavelength is in the range of about 1685 nm to 1700 nm.

13. An apparatus as in claim 11, wherein the methane concentration is less than or equal to approximately 50 ppm and the selected wavelength is one of approximately 1654 nm, approximately 1687 nm, approximately 1694 nm, and approximately 1697 nm.

14. An apparatus as in claim 11, wherein the methane concentration is in the range of approximately 1% to approximately 5% and the selected wavelength is in the range of about 1630 nm to 1660 nm.

15. An apparatus as in claim 11, wherein the methane concentration is in a range of approximately 1% to 5%, and the selected wavelength is one of approximately 1632 nm, approximately 1637.4 nm, 1640.4 nm, 1642.9 nm, 1645.5 nm, 1648.2 nm, 1650.9 nm, 1653.7 nm, and 1656.5 nm.

16. An apparatus as in claim 11, wherein the laser light source is a tunable diode laser.

17. An apparatus as in claim 16, wherein the laser light source is modulated based on a modulation signal provided by the microprocessor and wherein the microprocessor is configured to demodulate the direct current signal from the photodetector to generate a second harmonic signal that is analyzed to determine the intensity of light traversing the path length at the selected wavelength.

18. An apparatus as in claim 16, wherein the laser light source is selected from a vertical cavity surface emitting laser, a horizontal cavity surface emitting laser, a quantum cascade laser, a distributed feedback laser, and a color center laser.

19. An apparatus as in claim 11, further comprising a thermally controlled chamber that encloses one or more of the laser source, the photodetector, and the sample cell.

20. A method of detecting trace amounts of methane in carbon dioxide backgrounds, comprising:

directing a beam of light at a wavelength in the range of approximately 1630 nm to 100 nm through a gas mixture comprising carbon dioxide and less than approximately 5% methane, the selected wavelength coinciding with a methane absorption feature that is resolvable from an absorption background due to carbon dioxide, the beam of light being provided by a tunable diode laser;

quantifying an absorption at the selected wavelength in the gas mixture over a path length of less than or equal to approximately 50 cm; and

determining a methane concentration in the gas mixture based on the quantified absorption and a calibration function.