Portable nuclear moisture-density gauge with low activity nuclear sources

• US 4,766,319 A
• Filed: 02/12/1987
• Issued: 08/23/1988
• Est. Priority Date: 02/12/1987
• Status: Expired due to Term

• Current Assignee: Troxler Electronic Laboratories, Inc.
• Original Assignee: Troxler Electronic Laboratories, Inc.
• Inventors: Regimand, Ali
• Primary Examiner(s): Howell, Janice A.
• Assistant Examiner(s): NOT, DEFINED
• Application Number:
  US07/013,678
• Time in Patent Office: 558 Days
• Field of Search: 250/390 D, 250/390 E, 250/390 C, 250/390 R, 250/308, 250/358.1, 250/270, 250/391
• US Class Current: 250/390.05
• CPC Class Codes: G01N 23/02 by transmitting the radiation through the material

Abstract

The nuclear moisture-density gauge of the present invention employs a low activity neutron radiation source and a low activity gamma radiation source. In order to achieve more accurate density measurements at the relatively low count rates which results from the use of a low activity gamma source, the present invention is provided with means for generating a correction signal which is a function of the moisture content of the test material and which represents the amount of gamma radiation emitted from the test material resulting from the neutron capture reaction due to the presence of neutron capture elements, such as hydrogen, present in the test material. This correction signal is applied to the uncorrected density signal obtained from the gauge to thereby obtain a corrected density measurement which is unaffected by background gamma radiation caused by the presence of neutron capture elements in the test material. The gauge is also provided with means for correcting naturally occurring background gamma radiation from the test material.

Claims

1. A portable low activity nuclear measuring gauge for measuring the density and moisture characteristics of a test material, comprising

a low activity neutron radiation source for emitting fast neutrons into the test material,

thermal neutron detector means mounted in predetermined spaced relationship to said neutron source for detecting thermal neutrons which have been moderated by neutron moderating elements, such as hydrogen, present in the test material and for generating a signal representative of the moisture content of the test material,

a low activity gamma radiation source for emitting gamma radiation into the test material,

gamma radiation detector means mounted in predetermined spaced relationship to said gamma radiation source for detecting gamma radiation which is emitted from the gamma radiation source and which passes through the test material and for generating an uncorrected signal which is representative of the density of the test material plus error due to extraneous background radiation,

means operatively connected to said thermal neutron detector means for generating a correction signal which is a function of said moisture signal and which represents the amount of gamma radiation emitted from said test material resulting from the (n, γ

) neutron capture reaction due to the presence of neutron capture elements, such as hydrogen, in the test material; and

means for applying said correction signal to said uncorrected density signal to obtain a corrected density signal which is unaffected by background gamma radiation caused by the presence of neutron capture elements, such as hydrogen, in the test material.

2. A gauge according to claim 1 wherein said neutron radiation source has a radiation activity of less than 1000 microcuries.

3. A gauge according to claim 1 wherein said gamma radiation source has a radiation activity of less than 1000 microcuries.

4. A gauge according to claim 1 wherein said gamma radiation source and said neutron radiation source have a total radiation activity of no more than 100 microcuries.

5. A gauge according to claim 1 additionally including means for receiving and storing a second correction signal representative of natural background radiation present in the test material, and wherein said means for applying said correction signal to said density signal is also operable for applying said second correction signal to said density signal to thereby obtain a corrected density signal which is unaffected both by natural background radiation present in the test material and by background gamma radiation caused by the presence of neutron capture elements in the test material.

6. A method of measuring the density of a test material using a low activity gamma radiation source in the presence of a neutron radiation source, comprising:

directing fast neutrons from a neutron radiation source into the test material,

detecting neutrons which have been moderated and thermalized by neutron moderating elements present in the test material and generating a signal representative of the moisture content of the test material,

directing gamma radiation from a gamma radiation source into the test material,

detecting gamma radiation emitted from the gamma radiation source and which passes through the test material and generating an uncorrected signal which is representative of the density of the test material plus error due to extraneous background radiation,

generating a correction signal which is a function of said moisture signal and which represents the amount of gamma radiation emitted from said test material resulting from the (n, γ

) neutron capture reaction due to the presence of neutron capture elements, such as hydrogen, in the test material, and

applying said correction signal to said uncorrected density signal to obtain a corrected density signal which is unaffected by background gamma radiation caused by the presence of neutron capture elements in the test material.

7. A method according to claim 6 additionally including providing a second correction signal representative of natural background radiation present in the test material, and also applying said second correction signal to said uncorrected density signal to obtain a corrected density signal which is unaffected by both the natural background radiation present in the test material and by background gamma radiation caused by the presence of neutron capture elements in the test material.

8. A method according to claim 6 wherein said step of directing fast neutrons comprises directing neutrons from a low activity neutron source having a radiation activity of less than 1000 microcuries.

9. A method according to claim 6 wherein said step of directing gamma radiation comprises directing gamma radiation from a low activity gamma radiation source having a radiation activity of less than 1000 microcuries.

10. A method according to claim 6 wherein the neutrons and the gamma radiation are directed from radiation sources having a total radiation activity of no more than 100 microcuries.