Gamma ray prospecting system

• US 4,317,033 A
• Filed: 11/16/1979
• Issued: 02/23/1982
• Est. Priority Date: 06/15/1979
• Status: Expired due to Term

• Current Assignee: Hudson's Bay Oil and Gas Company Limited, Kenting Earth Sciences Limited
• Original Assignee: Hudson's Bay Oil and Gas Company Limited, Kenting Earth Sciences Limited
• Inventors: Panenka, Jaroslav R., Pavlik, Bohuslav, Olson, Daniel P.
• Primary Examiner(s): Smith, Alfred E.
• Assistant Examiner(s): Howell, Janice A.
• Application Number:
  US06/095,101
• Time in Patent Office: 830 Days
• Field of Search: 250/252, 250/253, 250/255, 250/336, 250/361 R, 250/366, 250/369
• US Class Current: 250/253
• CPC Class Codes: G01T 1/36 Measuring spectral distribution of X-rays or of nuclear radiation spectrometry pulse selection circuits per se H03K; investigation of materials by radiation diffraction G01N23/20; spectrometer tubes H01J49/00
• CPC Class Codes: G01V 5/025 specially adapted for use from aircraft

Abstract

A means and method for distinguishing full energy absorption peaks from background energy in a gamma ray prospecting system. Photopeaks in the received energy spectrum are determined, and boundaries to the peaks are located. The energy within the boundaries assuming a predetermined curve between the boundaries is integrated. The filtered energy within the actual photopeak curve is also integrated, and the two integrated signals are subtracted to provide a signal representative of the net photopeak area or amplitude. This peak area (or amplitude) is directly proportional to intensity of gamma radiation due to uranium, thorium and potassium in the ground. This signal is displayed and continuously updated on a cathode ray tube as a function of time.

Claims

1. Means for distinguishing full energy absorption peaks received across an energy band from background energy at a particular physical location comprising:

(a) means for receiving a gamma ray energy spectrum of radiation,

(b) means for distinguishing the peak energy level within an energy band of said spectrum, and for integrating said energy within said band,

(c) means for distinguishing a statistical value of the background gamma radiation within said band, and for integrating the background radiation within said band,

(d) means for subtracting the integrated statistical value of background energy from the integrated peak energy, and

(e) means for providing an output signal representative of the difference of the integrated peak energy level and said integrated statistical value within said band, to provide an indication of the presence of radiation emissive mineral at said particular location.

2. Means for distinguishing photopeaks of energy received across an energy band from background energy as defined in claim 1 in which said energy is continuously received from a plurality of juxtaposed and continuous physical locations, means for storing predetermined periods of said energy relating to said plurality of physical locations and means for applying serially said predetermined periods of said energy both said means for distinguishing as set forth in paragraphs (b) and (c) of claim 1.

3. means for distinguishing photopeaks of energy received across an energy band from background energy as defined in claim 2, in which said output signal is of the form indicative of levels of radiation emissive minerals sequentially related directly to said plurality of physical locations.

4. Means for distinguishing photopeaks of energy received across an energy band from background energy at a particular physical location as defined in claim 1 or 2, further including means for displaying the output signal as an amplitude as a function of the energy spectrum.

5. Means for distinguishing photopeaks of energy received across an energy band from background energy as defined in claim 3 further including means for continuously displaying the output signal as an amplitude as a function of the energy spectrum.

6. Means for distinguishing photopeaks of energy received across an energy band from Compton background energy at a particular physical location as defined in claim 1, in which the received energy is passed through a filter to obtain said integrated value of Compton energy, in which the filter has the transfer characteristics ##EQU5## where A_N is the received energy level in a particular window,

N is the window number and

K₀, K₁, K₂ and K₃ are constants.

7. Means for distinguishing photopeaks of energy received across an energy band from Compton background energy at a particular physical location as defined in claim 6 in which

K₀ =1.0

K₁ =0.9

K₂ =0.75 and

K₃ =0.5.

8. Means for distinguishing full energy absorption peaks received across an energy band from background energy at a particular physical location comprising:

(a) means for receiving a gamma ray energy spectrum of radiation,

(b) means for distinguishing full energy absorption peaks of said received energy,

(c) means for filtering the received energy,

(d) means for defining a lower and an upper filtered spectrum window boundary of at least one of said peaks,

(e) means for determining the amplitude of the energy at said boundaries,

(f) means for integrating the energy between said boundaries, with a predetermined energy change between the energy amplitudes at said boundaries, to obtain a signal representative of the background energy,

(g) means for integrating the filter-d energy amplitude between said boundaries, to obtain a total photopeak area signal, and

(h) means for subtracting the signal representative of the background energy from the total photopeak area signal to obtain a signal representative of the net photopeak area within the spectrum window.

9. Means for distinguishing full energy absorption peaks received across an energy band from background energy as defined in claim 8, further including means for continuously displaying updated said net photopeak areas as an ordinate bar on an abcissa representative of the spectrum window as the means for receiving radiation is passed over a land area.

10. Means for distinguishing full energy absorption peaks received across an energy band from background energy as defined in claim 9 in which the means for receiving radiation is comprised of a spectrometer.

11. Means for distinguishing full energy absorption peaks received across an energy band from background energy as defined in claim 10 in which the means for defining the upper and lower boundaries includes means for differentiating the received energy on the upper and lower energy sides of the energy absorption peak and determining spectrum locations where the energy curve changes sign.

12. Means for distinguishing full energy absorption peaks received across an energy band from background energy as defined in claim 8 in which the filter means is a recursive filter.

13. Means for distinguishing full energy absorption peaks received across an energy band from background energy as defined in claim 9, 10 or 12 further including an analog-to-digital converter having its input connected to the output of the spectrometer, a microcomputer having its data input connected to the output of the analog-to-digital converter, an oscilloscope displaying means having its input connected to the output of the microcomputer, the microcomputer being adapted to form said means for filtering, said means for defining said boundaries, said means for determining the amplitude of the energy at said boundaries, said means for integrating, said means for subtracting, and said further means for driving said displaying means.

14. A method for distinguishing full energy absorption peaks across an energy band from background energy comprising:

(a) receiving an energy spectrum signal at least within the energy band to be distinguished,

(b) filtering the signal,

(c) defining at least one of said peaks,

(d) defining upper and lower spectrum boundaries to said one peak,

(e) determining the amplitudes of said filtered signal at said boundaries,

(f) assigning a predetermined change in amplitude of said filtered signal between said amplitudes of said filtered signal,

(g) integrating the signal between said boundaries from said amplitudes and predetermined change in amplitude to obtain a signal representative of background energy,

(h) integrating the filtered signal between said boundaries to obtain a signal representative of total photopeak area,

(i) subtracting the background energy signal from the total photopeak area signal to obtain a net photopeak signal.

15. A method of distinguishing full energy absorption peaks across an energy band from background energy as defined in claim 14, in which said predetermined change in amplitude is linear.

16. A method of distinguishing full energy absorption peaks across an energy band from background energy as defined in claim 14, in which said predetermined change in amplitude is cubic.

17. A method of distinguishing full energy absorption peaks across an energy band from background energy as defined in claim 14, in which said predetermined change in amplitude is a smoothed polynomial curve.

18. A method of distinguishing full energy absorption peaks across an energy band from background energy as defined in claim 14, 15, or 17, further including the step of displaying the photopeak signal as a function of a spectrum window.