Portable remote laser sensor for methane leak detection

• US 4,489,239 A
• Filed: 09/24/1982
• Issued: 12/18/1984
• Est. Priority Date: 09/24/1982
• Status: Expired due to Fees

• Current Assignee: United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration
• Original Assignee: United States Of America As Represented By The Administrator Of The National Aeronautics And Space Administration
• Inventors: Grant, William B., Hinkley, E. David Jr.
• Primary Examiner(s): Howell, Janice A.
• Application Number:
  US06/423,016
• Time in Patent Office: 816 Days
• Field of Search: 250/338 R, 250/339, 250/343, 356/437, 356/414
• US Class Current: 250/339.03
• CPC Class Codes: G01J 2001/4242 Modulated light, e.g. for synchronizing source and detector circuit
• CPC Class Codes: G01N 2021/395 using a topographic target
• 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 21/39 using tunable lasers

Abstract

A portable laser system for remote detection of methane gas leaks and concentrations is disclosed. The system transmitter includes first and second lasers, tuned respectively to a wavelength coincident with a strong absorption line of methane and a reference wavelength which is weakly absorbed by methane gas. The lasers are aimed at a topographical target along a system axis and the beams successively interrupted by a chopper wheel.

The system receiver includes a spherical mirror for collecting the reflected laser radiation and focusing the collected radiation through a narrowband optical filter onto an optial detector. The filter is tuned to the wavelength of the two lasers, and rejects background noise to substantially improve the signal-to-noise ratio of the detector. The output of the optical detector is processed by a lock-in detector synchronized to the chopper, and which measures the difference between the first wavelength signal and the reference wavelength signal.

Claims

1. A portable, low wattage system for remotely detecting methane gas concentrations in the atmosphere from radiation reflected from a topographical target, said radiation including thermal and solar-type background noise, including methane-related laser wavelengths to be analyzed, said system comprising:

means for generating a first laser beam at a first wavelength coincident with a natural absorption line of methane gas;

means for generating a second laser beam at a second wavelength which is not a strong absorption line of methane gas;

means for successively interrupting said first and second laser beams;

means for directing said first and second laser beams at a topographical target;

collecting means for focusing a portion of said reflected laser radiation;

narrowband optical filter means centered near said first and second wavelengths for passing said focused radiation, including the wavelengths to be analyzed and for effectively reducing said thermal and solar-type background noise;

optical detector means for detecting the intensity of incident laser radiation and generating a detector signal representative of such intensity;

signal processing means synchronized to the operation of said means for interrupting said laser beams for performing processing of the data from said optical detector to effectively cancel out the background noise while providing an output signal indicative of the relative intensity of said radiation at said first wavelength.

2. The system of claim 1 wherein said first wavelength is about 3.3922 μ

m and said means for generating said first wavelength comprises a first Helium Neon laser.

3. The system of claim 1 wherein said first and second wavelengths are within one cm^-1 (0.001 μ

m) of each other.

4. The system of claim 3 wherein said second wavelength is about 3.3911 μ

m and said means for generating a second laser beam comprises a second Helium Neon laser.

5. The system of claim 4 wherein a cell containing CH₄ is disposed in the optical cavity of said second laser.

6. The system of claim 1 wherein said interrupting means is adapted to interrupt said first and second laser beams 180°

out-of-phase, wherein only said first laser beam is passed during a first portion of the cycle of the interrupting means, and only said second laser beam is passed during the succeeding portion of said cycle.

7. The system of claim 6 wherein said signal processing means is adapted to integrate said detector signal over said first portion of said cycle to form a first summed signal and to integrate said detector signal over said second portion of said cycle to form a second summed signal.

8. The system of claim 7 wherein said signal processing means is further adapted to form a difference signal P representative of the difference between said first summed signal and said second summed signal.

9. The system of claim 1 wherein said signal processing means is adapted such that said detector signal is determined, when 2α

(cl+CR)<

<

1, in accordance with the following expression;

##EQU8## where A is the area (cm²) of the optical detector, ρ

is the reflectance of said topographical target, l is the optical detector efficiency, Δ

α

is the differential absorption coefficient (atm^-1 cm^-1), c is the concentration of gas in the methane gas plume (atm or ppm), l is the diameter of the plume(cm), C is the ambient concentration of the gas (atm) and R is the distance from the optical detector to the topographical target (cm).

10. The system of claim 1 further comprising cooling means for cooling said optical detector and said optical filter means.

11. The system of claim 10 wherein said cooling means is adapted to cool said detector and said optical filter to about 77K.

12. The system of claim 1 wherein said optical detector means is adapted to detect incident laser radiation having wavelengths from 1 μ

m to 4 μ

m.

13. The system of claim 1 wherein said collector means is adapted to focus said incident laser radiation at an image plane, and said optical detector means is disposed at said image plane.

14. The system of claim 1 wherein said narrowband filter means is centered at about 3.4 μ

m and its power transmission points are at about ±

0.07 μ

m on each side of said center.

15. The system of claim 1 wherein said collecting means comprises a spherical mirror.

16. The system of claim 15 wherein said optical detector means is disposed between said spherical mirror and said topographical target.

17. The system of claim 1 wherein said collecting means comprises a Fresnel lens means.

18. A portable, low wattage system for detecting methane gas concentrations in the atmosphere from reflected laser radiation which includes methane wavelengths to be analyzed and thermal, solar or room light background noise, said system comprising:

laser means adapted for selectively generating a laser beam at either a first wavelength coincident with a natural absorption line of methane gas or at a second wavelength which is not a strong absorption line of methane gas;

control means coupled to said laser means for alternatively selecting said laser beam at said first wavelength and then said seond wavelength;

means for directing said laser means at a topographical target;

collecting means for focusing a portion of the laser radiation and background noise reflected from said target;

narrowband optical filter means centered near said first wavelength for passing said focused first and second wavelengths of laser radiation and effectively reducing said background noise by a factor of up to four;

optical filter means responsive to the signals passed through said narrowband optical filter means for detecting the intensity of incident laser radiation and generating a detector signal representative of such intensity; and

signal processing means synchronized to the operation of said selecting means for processing the data from said optical detector and providing an output signal indicative of the relative intensity of said laser radiation at said first wavelength.

19. The system of claim 18 wherein said laser means includes a plasma cavity having Brewster angle windows and further including a Fabry-Perot interferometer disposed on a piezoelectric disc, said disc being driven by oscillator means, whereby for one position of said disc, the laser produces a laser beam at said first wavelength, and for a second position of said disc means, said laser means produces a laser beam at said second wavelength.

20. The system of claim 19 wherein said signal processing means is synchronized to the operation of said oscillator means.

21. The system of claim 19 wherein the portability of the system results from the system'"'"'s total weight of around 25 pounds, and the low wattage required by the system is in the area of 40 watts of electrical power, said system further comprising a battery for supplying said wattage to remotely and portably sense methane leaks.