Method and apparatus for measuring wall thickness of a vessel

• US 20050254614A1
• Filed: 03/11/2005
• Published: 11/17/2005
• Est. Priority Date: 03/11/2004
• Status: Abandoned Application

• Current Assignee: Clear Path Technologies Incorporated
• Original Assignee: Clear Path Technologies Incorporated
• Inventors: McKinny, Kevin Scott
• Application Number:
  US11/078,688
• Publication Number:
  US 20050254614A1
• Time in Patent Office: Days
• US Class Current: 376/159
• CPC Class Codes: G01B 15/02 for measuring thickness
• CPC Class Codes: G01N 23/2257 Measuring excited X-rays, i.e. particle-induced X-ray emission [PIXE]
• CPC Class Codes: G21C 17/003 Remote inspection of vessels, e.g. pressure vessels
• CPC Class Codes: Y02E 30/30 Nuclear fission reactors

Abstract

A method measures a thickness of a wall. The method includes irradiating at least a portion of the wall with a plurality of 14-MeV neutrons. The wall emits gamma rays with photon energies characteristic of the atomic nuclei in response thereto. The method further includes detecting at least a portion of the gamma rays emitted from the wall and measuring the photon energies of the detected gamma rays with an energy resolution better than approximately 0.5%. The detected gamma rays have a first range of photon energies. The method further includes selecting a second range of photon energies which is a subset of the first range of photon energies. The method further includes calculating a number of detected gamma rays having measured photon energies within the selected second range of photon energies. The method further includes determining the wall thickness using the calculated number of detected gamma rays.

Claims

1. A method of measuring a thickness of a wall, the method comprising:

irradiating at least a portion of the wall with a plurality of 14-MeV neutrons, the wall emitting gamma rays with photon energies characteristic of the atomic nuclei in response thereto;

detecting at least a portion of the gamma rays emitted from the wall and measuring the photon energies of the detected gamma rays with an energy resolution better than approximately 0.5%, the detected gamma rays having a first range of photon energies;

selecting a second range of photon energies which is a subset of the first range of photon energies;

calculating a number of detected gamma rays having measured photon energies within the selected second range of photon energies; and

determining the wall thickness using the calculated number of detected gamma rays.

2. A method of measuring a thickness of a wall, the method comprising:

irradiating at least a portion of the wall with a plurality of neutrons, the wall emitting gamma rays with photon energies characteristic of the atomic nuclei in response thereto;

detecting at least a portion of the gamma rays emitted from the wall and measuring the photon energies of the detected gamma rays, the detected gamma rays having a first range of photon energies;

selecting a second range of photon energies which is a subset of the first range of photon energies;

calculating a number of detected gamma rays having measured photon energies within the selected second range of photon energies; and

determining the wall thickness using the calculated number of detected gamma rays.

3. The method of claim 2, wherein the atomic nuclei absorb neutrons and emit delayed nuclear-decay gamma rays.

4. The method of claim 2, wherein the neutrons have energies approximately equal to 14 MeV.

5. The method of claim 2, wherein the neutrons are generated by a fast neutron emitter source.

6. The method of claim 2, wherein the neutrons are generated by a deuterium-tritium reaction.

7. The method of claim 2, wherein the wall comprises concrete or cement.

8. The method of claim 2, wherein the wall comprises a pipe wall.

9. The method of claim 2, wherein the wall has a known initial wall thickness greater than the determined wall thickness, the method further comprising determining an amount of erosion of the wall by calculating a difference between the known initial wall thickness and the determined wall thickness.

10. The method of claim 2, wherein detecting the gamma rays comprises using a solid-state germanium detector.

11. The method of claim 10, wherein the solid-state germanium detector has an energy resolution better than 0.5%.

12. The method of claim 10, wherein the solid-state germanium detector has an energy resolution better than 0.3%.

13. The method of claim 2, wherein the neutrons are directed at the wall from a first side of the wall and gamma rays are detected from the first side of the wall.

14. The method of claim 2, wherein the neutrons are directed at the wall from a first side of the wall and gamma rays are detected from a second side of the wall.

15. The method of claim 2, wherein irradiating at least a portion of the wall with a plurality of neutrons comprises generating a plurality of neutron/alpha particle pairs from a target, each pair comprising a neutron and a corresponding alpha particle propagating in substantially opposite directions, the neutrons propagating toward the wall, the alpha particles propagating away from the wall.

16. The method of claim 2, wherein the gamma rays are emitted from nuclei of aluminum or maganese.

17. The method of claim 2, wherein the gamma rays are emitted from nuclei which, upon absorbing neutrons, become radioisotope nuclei which decays thereby emitting the gamma rays.

18. A method for measuring a thickness of a wall, the method comprising:

positioning a source of neutrons in proximity to the wall;

directing the neutrons at the wall, the neutrons causing the wall to emit gamma rays with photon energies characteristic of atomic nuclei within the wall;

detecting at least a portion of the gamma rays;

determining a photon energy distribution of the detected gamma rays; and

calculating the thickness of the wall from a subset of the photon energy distribution of the detected gamma rays.

19. The method of claim 18, wherein detecting at least a portion of the gamma rays comprises positioning a gamma ray detector in proximity to the wall.

20. The method of claim 19, wherein the gamma ray detector comprises a germanium detector.

21. The method of claim 20, wherein the germanium detector has an energy resolution better than 0.5%.

22. The method of claim 20, wherein the germanium detector has an energy resolution better than 0.3%.

23. The method of claim 18, wherein calculating the thickness of the wall comprises calculating a number of detected gamma rays having photon energies within the subset of the photon energy distribution.

24. The method of claim 18, wherein directing the neutrons at the wall comprises generating a plurality of neutron/alpha particle pairs from a target in the source, each pair comprising a neutron and a corresponding alpha particle propagating in substantially opposite directions, the neutrons propagating toward the wall, the alpha particles propagating away from the wall.

25. The method of claim 18, wherein the gamma rays are emitted from nuclei of aluminum or maganese.

26. The method of claim 18, wherein the gamma rays are emitted from nuclei which, upon absorbing a neutron, become a radioisotope nucleus which decays thereby emitting a gamma ray.

27. The method of claim 18, wherein the wall comprises concrete or cement.

28. The method of claim 18, wherein the wall is a portion of an above-ground structure.

29. The method of claim 28, wherein the structure comprises an oil pipeline.

30. The method of claim 18, wherein the wall has a known initial wall thickness greater than the determined wall thickness, and the method further comprises determining an amount of erosion of the wall by calculating a difference between the known initial wall thickness and the determined wall thickness.

31. The method of claim 18, wherein the energy of the neutrons is approximately equal to 14 MeV.

32. The method of claim 18, wherein the neutrons are generated by a deuterium-tritium reaction.