Method and apparatus for detecting a tracer gas using a single laser beam

• US 4,853,543 A
• Filed: 04/29/1987
• Issued: 08/01/1989
• Est. Priority Date: 09/13/1983
• Status: Expired due to Fees

• Current Assignee: Skyborne Exploration Corporation
• Original Assignee: Phillip Ozdemir
• Inventors: Ozdemir, Phillip
• Primary Examiner(s): Fields, Carolyn E.
• Assistant Examiner(s): NOT, DEFINED
• Application Number:
  US07/043,962
• Time in Patent Office: 825 Days
• Field of Search: 250/338.5, 250/345, 250/372, 356/402, 356/407, 356/434, 356/438, 356/342, 356/301, 356/51, 356/416
• US Class Current: 250/372
• CPC Class Codes: G01N 2021/394 DIAL method
• CPC Class Codes: G01N 2021/395 using a topographic target
• CPC Class Codes: G01N 21/39 using tunable lasers
• CPC Class Codes: G01V 9/007 by detecting gases or particles representative of underground layers at or near the surface analysing earth materials G01N33/24; analysing gases per se G01N

Abstract

A method and apparatus for airborne prospecting for base and precious metal deposits, petroleum and natural gas deposits, geothermal steam deposits, and leaks in natural gas pipelines. A trace gas associated with the deposits in the near-surface atmosphere is detected with a differential absorption optical technique utilizing only a single laser beam to perform remote differential optical measurement. Anomalies in the tracer gas, which are indicative of underground deposits, are detected by transmiting a laser beam having narrow linewidth laser pulses at a high repetition rate with a center wavelength approximately equal to the atomic absorption line of the tracer gas to the area under investigation. The pulses are directed toward the investigated area from an airborne platform, reflected off the ground, and are collected by a detector on the airborne platform. Each pulse received is then broken down into a portion containing energy which is coincident with the absorption line of the tracer gas and a portion which is non-coincident with the absorption line of the tracer gas using a special optical filter. A tracer gas cell removes all the energy from the pulse which is coincident with the tracer gas absorpotion line, and the energy detected from the tracer gas cell corresponds to the amount of energy in the pulse which is off-resonance. By subtracting the off-resonance energy from the total energy received, it is possible to calculate the energy in the pulse which is received in the on-resonance spectral interval.

Claims

1. A method of detecting a target gas having a predetermined atomic absorption line, comprising the steps of:

generating a beam of laser radiation having a spectral bandwidth including, while being broader than, said predetermined atomic absorption line of said target gas;

transmitting said beam of laser radiation toward an area to be investigated for said target gas;

splitting the beam reflected from said area into first and second portions, said first portion including the radiation in said reflected beam in the spectral region coinciding with said predetermined atomic absorption line as an on-resonance beam, and said second portion including only the radiation in said reflected beam in the spectral region outside of said spectral region coinciding with said predetermined atomic absorption line as an off-resonance beam;

measuring the intensities of said on-resonance beam and said off-resonance beam and producing an on-resonance energy signal and an off-resonance energy signal, respectively related thereto; and

determining the absolute concentration of the target gas in said area from the measured intensities.

2. A method as in claim 1, wherein said target gas is mercury (Hg).

3. A method as in claim 1, wherein said laser radiation is in the ultraviolet spectral region.

4. A method as in claim 1, wherein said generating step includes the steps of:

pumping a dye laser with an excimer laser; and

doubling the frequency of the dye laser light to coincide with said predetermined atomic absorption line of said target gas.

5. A method as in claim 1, including the further steps of:

tapping off a portion of the generated beam of laser radiation as a reference laser beam;

splitting the reference laser beam into two approximately equal portions;

measuring the total pulse energy in one portion of said reference laser beam;

removing part of the energy in the other portion of said reference laser beam which is coincident with the predetermined atomic absorption line of said target gas in a calibration cell; and

measuring the pulse energy remaining in the other portion of said reference laser beam after it has passed through said calibration cell.

6. A method as in claim 5, wherein said calibration cell contains a known quantity of said target gas for determining the effective absorption cross-section of said target gas.

7. A method as in claim 5, wherein said reflected beam splitting step includes the steps of:

splitting the reflected beam into two portions;

measuring the pulse energy of one portion of said reflected beam;

passing the other portion of said reflected beam through an optical cell containing a saturated volume of said target gas at a regulated temperature, said optical cell absorbing the optical energy in the other portion of said reflected beam which is coincident with the predetermined atomic absorption line of said target gas;

measuring the pulse energy remaining in the other portion of said reflected beam after it has passed through said optical cell as said off-resonance energy signal; and

subtracting said off-resonance energy signal from the measured pulse energy of said one portion of said reflected beam to get said on-resonance energy signal.

8. A method as in claim 7, wherein said target gas concentration determining step includes the steps of:

generating an indication of the distance said transmitted laser beam travels; and

determining the target gas concentration N_atmos in accordance with the following equation;

##EQU2## where;

N_atmos =Concentration of detected target gas in parts per billion,

N_cell =Concentration of target gas in calibration cell in parts per billion,

L=Length of calibration cell in meters,

R=Distance to area being investigated for target gas,

P=Received power of on-resonance energy signal in watts,

P'"'"'=Received power of off-resonance energy signal in watts,

Pc=On-resonance power of said reference laser beam in watts, and

Pc'"'"'=Off-resonance power of said reference laser beam from said calibration cell in watts.

9. A method as in claim 8, wherein said distance indication generating step includes the steps of:

measuring the time between transmitting said laser beam and measuring said reflected laser beam; and

relating said time to distance.

10. A method as in claim 1, including the further step of monitoring the position of said area being investigated.

11. A method as in claim 10, including the further step of storing data related to the concentration of said target gas and the position at which said concentration was measured.

12. A method as in claim 1, including the further step of displaying in real time the concentration of said target gas.

13. A method as in claim 1, including the further step of correlating the magnitude of the concentration of said target gas detected with the existence of one of precious metals deposits, petroleum and natural gas deposits, geothermal steam deposits, and leaks in natural gas pipelines.

14. A method as in claim 1, wherein said steps are performed aboard an airborne platform.

15. A method of locating an underground deposit by detecting the presence of mercury gas, comprising the steps of:

(a) generating a beam of ultraviolet laser radiation having a spectral region about a center frequency which coincides with an atomic absorption line of the mercury (Hg) atom;

(b) transmitting said beam of laser radiation toward an area being investigated for the presence of mercury gas;

(c) measuring the intensity of the transmitted laser beam;

(d) detecting said beam of laser radiation after it has been reflected from said area;

(e) splitting the detected beam into first and second portions;

(f) measuring the pulse energy of said first portion of the detected beam;

(g) passing said second portion of the detected beam through a mercury vapor-filled optical cell, said optical cell being kept at a regulated temperature, and said mercury vapor in said optical cell absorbing the optical energy in said second portion of the detected beam which is coincident with the atomic absorption line of mercury;

(h) measuring the pulse energy remaining in said second portion of the detected beam after it has passed through said optical cell as an off-resonance energy signal;

(i) subtracting said off-resonance energy signal from the measured pulse energy of said first portion of the detected beam to get an on-resonance energy signal;

(j) measuring the intensities of said on-resonance energy signal and said off-resonance energy signal;

(k) generating an indication of the distance said transmitted laser beam travels to said area;

(l) determining the concentration of said mercury gas in said area employing the results of steps (c), (j) and (k);

(m) relating said mercury gas concentration to the existence of said underground deposit;

(n) displaying said mercury gas concentration in real time;

(o) determining the position of said area being investigated; and

(p) storing said mercury gas concentration with the position at which said mercury gas concentration was measured.

16. A method as in claim 15, wherein said steps (a) through (p) are performed aboard an airborne platform.

17. An apparatus for detecting a target gas having a predetermined atomic absorption line, comprising:

means for generating a beam of laser radiation having a spectral bandwidth including, while being broader than, said predetermined atomic absorption line of said target gas;

means, responsive to said generating means, for transmitting said beam of laser radiation toward an area to be investigated for said target gas;

means for splitting said beam after it has been reflected from said area into first and second portions, said first portion including the radiation in said reflected beam in the spectral region coinciding with said predetermined atomic absorption line as an on-resonance beam, and said second portion including only the radiation in said reflected beam in the spectral region outside of said spectral region coinciding with said predetermined atomic absorption line as an off-resonance beam; and

processing means, responsive to said first and second portions of said reflected beam, for measuring the intensities of said on-resonance beam and said off-resonance beam and for determining the absolute concentration of the target gas in said area from the measured intensities.

18. An apparatus according to claim 17, wherein said generating means generates radiation having a spectral bandwidth including the atomic absorption line of mercury (Hg).

19. An apparatus according claim 17, wherein said generating means generates laser radiation in the ultraviolet spectral region.

20. An apparatus according to claim 17, wherein said generating means comprises:

an excimer laser;

a dye laser which is pumped by said excimer laser; and

frequency doubling means for doubling the frequency of the dye laser output to coincide with said predetermined atomic absorption line of said target gas.

21. An apparatus according to claim 20, wherein said frequency doubling means includes a potassium pentaborate crystal.

22. An apparatus according to claim 20, wherein said frequency doubling means includes a Raman cell.

23. An apparatus according to claim 17, further comprising calibration means for determining the intensity of the transmitted laser beam, said calibration means comprising:

means for tapping off a portion of the generated beam of laser radiation as a reference laser beam;

means for splitting the reference laser beam into two approximately equal portions;

means for measuring the total pulse energy in one portion of said reference laser beam;

a calibration cell for removing a portion of the energy in the other portion of said reference laser beam which is coincident with the predetermined atomic absorption line of said target gas; and

means for measuring the pulse energy remaining in the other portion of said reference laser beam after it has passed through said calibration cell.

24. An apparatus according to claim 23, wherein said calibration cell contains a known quantity of said target gas for determining the effective absorption cross-section of said target gas.

25. An apparatus according to claim 23, wherein said means for splitting the reflected beam comprises:

filtering means containing a saturated volume of said target gas at a regulated temperature for absorbing the optical energy in one portion of said detected beam which is coincident with the predetermined atomic absorption line of said target gas; and

said processing means comprises;

means for measuring the total pulse energy of the other portion of said reflected beam, and

means for measuring the pulse energy remaining of said one portion of said reflected beam after it has passed through said filtering means.

26. An apparatus according to claim 25, wherein said filtering means includes a mercury vapor-filled optical cell and said target gas is mercury (Hg).

27. An apparatus according to claim 25, wherein said processing means includes:

means for generating a value related to the distance between said transmitting means and said area; and

means for determining the target gas concentration N_atmos in accordance with the following equation;

##EQU3## where;

N_atmos =Concentration of detected target gas in parts per billion,

N_cell =Concentration of target gas in calibration cell in parts per billion,

L=Length of calibration cell in meters,

R=Distance to area being investigated for target gas,

P=Received power of on-resonance energy signal in watts,

P'"'"'=Received power of off-resonance energy signal in watts,

Pc=On-resonance power of said reference laser beam in watts, and

Pc'"'"'=Off-resonance power of said reference laser beam from said calibration cell in watts.

28. An apparatus according to claim 17, further comprising means for monitoring the position of said area being investigated.

29. An apparatus according to claim 28, wherein said position monitoring means includes a navigation receiver.

30. An apparatus according to claim 28, further comprising means for storing data related to the concentration of said target gas and the position at which said concentration was measured.

31. An apparatus according to claim 17, further comprising means for displaying in real time the concentration of said target gas.

32. An apparatus according to claim 17, further comprising means for detecting said beam of laser radiation after it has been reflected, said detecting means comprising:

a detector for receiving said reflected laser beam;

trigger generating means, coupled to said detector, for sensing the reception of a reflected laser beam; and

analog-to-digital converting means, coupled to said detector and said trigger generating means, for converting the output of said detector in response to an indication from said trigger generating means.

33. An apparatus according to claim 17, further comprising an airborne platform on which said generating means, transmitting means and splitting means are disposed.

34. An apparatus for locating an underground deposit by detecting the presence of mercury gas, comprising:

means for generating a beam of ultraviolet laser radiation having a spectral region about a center frequency which coincides with an atomic absorption line of the mercury (Hg) atom;

means, responsive to said generating means, for transmitting said beam of laser radiation toward an area being investigated for the presence of mercury gas;

means for measuring the intensity of the transmitted laser beam;

means for detecting said beam of laser radiation after it has been reflected from said area;

means for splitting the detected beam into first and second portions;

means for measuring the pulse energy of said first portion of said detected beam;

a mercury vapor-filled optical cell kept at a regulated temperature for absorbing the optical energy in said second portion of said detected beam which is coincident with the atomic absorption line of mercury;

means for measuring the pulse energy remaining in said second portion of said detected beam after it has passed through said optical cell as an off-resonance energy signal;

processing means, responsive to said first and second portions of said detected beam, for subtracting said off-resonance energy signal from the measured pulse energy of said first portion of said detected beam to get an on-resonance energy signal;

for measuring the intensities of said on-resonance energy signal and said off-resonance energy signal;

for generating an indication of the distance said transmitted laser beam travels to said area;

for determining the concentration of said mercury gas in said area in response to the outputs of said means for measuring the intensity of the transmitted laser beam, said means for measuring the intensities of said on-resonance energy signal and said off-resonance energy signal, and said means for generating an indication of the distance said transmitted laser beam travels to said area; and

for relating said mercury gas concentration to the existence of said underground deposit;

means for displaying said mercury gas concentration in real time;

means for determining the position of said area being investigated; and

means for storing said mercury gas concentration with the position at which said mercury gas concentration was measured.

35. An apparatus according to claim 34, further comprising an airborne platform on which said generating means, transmitting means and detecting means are disposed.