Elemental analysis using temporal gating of a pulsed neutron generator
US-2015323473-A1 · Nov 12, 2015 · US
US9528952B1 · US · B1
| Field | Value |
|---|---|
| Publication number | US-9528952-B1 |
| Application number | US-201615156757-A |
| Country | US |
| Kind code | B1 |
| Filing date | May 17, 2016 |
| Priority date | May 17, 2016 |
| Publication date | Dec 27, 2016 |
| Grant date | Dec 27, 2016 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
A method of determining structural defects in a component that utilizes neutron activation of a solution having the ability to penetrate small cracks on the surface of a material via capillary absorption that produces a discernable prompt gamma release of a defined energy when exposed to a neutron pulse. The intensity of the gamma rays produced at the desired energy at a user controlled position on the surface is used to determine the crack location, length and depth.
Opening claim text (preview).
What is claimed is: 1. A method of nondestructively detecting a structural defect in a surface of an irradiated material comprising the steps of: applying a mixture of a noncorrosive crack penetrant including chemical species that have relatively large cross-sections for fast neutron induced prompt gamma emission interactions of a defined energy to the surface of the material to be examined; irradiating the surface of the material with a neutron pulse generator; positioning a plurality of beta radiation detectors tuned to the defined energy of photo-electrically produced electrons generated in an electron generating window located between an active region of the detector and the surface being examined, in a regular pattern over the surface of the material to which the mixture is applied, the plurality of beta radiation detectors respectively providing an output indicative of a reception of the prompt gamma release of the defined energy in an area of the surface viewed by a corresponding one of the beta radiation detectors; and employing the receptions to map a characteristic of the defect. 2. The method of claim 1 wherein the characteristic is a location and length of the defect on the surface. 3. The method of claim 1 wherein the characteristic is a depth of the defect on the surface. 4. The method of claim 3 wherein the depth of the defect is determined from the strength of the reception. 5. The method of claim 1 wherein the mixture is absorbed into the defect by capillary absorption. 6. The method of claim 1 wherein the neutron pulse generator is a neutristor style Neutron Pulse Generator. 7. The method of claim 1 wherein the tuning of the beta radiation detectors is accomplished by placing a high atomic number sacrificial material between the surface being examined and an active portion of the beta radiation deteaors to act as an electron radiator. 8. The method of claim 7 wherein the beta radiation detectors are silicon carbide (SiC) detectors. 9. The method of claim 8 wherein the thickness, distance from the active detector region, and type of material used in the sacrificial layer of the beta radiation detector is selected to ensure that mostly the electrons produced by Photoelectric Absorption by the desired emitted prompt gamma radiation energy are completely stopped inside the active region of the SiC detectors. 10. The method of claim 7 wherein the sacrificial material is either platinum or tungsten. 11. Apparatus for nondestructively detecting and characterizing flaws in the surface of an irradiated material comprising; a spray system configured to spray a mixture of a noncorrosive crack penetrant either having a high Nitrogen content, or one that is mixed with a chemical species having a large portion of an isotope that has a relatively large fast neutron prompt capture gamma emission cross section of a defined energy of photoelectric to the surface of the material to be examined; a neutron pulse generator configured to irradiate a surface of the material; a plurality of beta radiation detectors, tuned to the defined energy of photo-electrically produced electron energy generated in an electron generating window located between an active region of the beta radiation detectors and the surface being examined, the beta radiation detectors positioned in a predetermined pattern over the surface of the material to which the mixture is applied, the plurality of beta radiation detectors respectively providing an output indicative of a reception of the prompt gamma release of the defined energy in an area of the surface viewed by a corresponding one of the beta radiation detectors; and a beta radiation detector output from which the receptions can be employed to map a characteristic of the defect. 12. The apparatus of claim 11 wherein the characteristic is a location and length of the defect on the surface. 13. The apparatus of claim 11 wherein the characteristic is a depth of the defect on the surface. 14. The apparatus of claim 13 wherein the depth of the defect is determined from the strength of the reception. 15. The apparatus of claim 11 wherein the mixture is absorbed into the defect by capillary absorption. 16. The apparatus of claim 11 wherein the neutron pulse generator is a neutristor style Neutron Pulse Generator. 17. The apparatus of claim 11 wherein the beta radiation detectors include a high atomic number sacrificial material between the surface being examined and an active portion of the beta radiation detectors to act as an electron radiator. 18. The apparatus of claim 17 wherein the beta radiation detectors are SiC detectors. 19. The apparatus of claim 18 wherein the thickness, distance from the active detector region, and type of material used in the sacrificial layer of the beta radiation detector is selected to ensure that mostly the electrons produced by Photoelectric Absorption by the desired emitted prompt gamma radiation energy are completely stopped inside the active region of the Sic detectors. 20. The apparatus of claim 17 wherein the sacrificial material is either platinum or tungsten.
using neutron activation analysis [NAA] · CPC title
using opaque penetrant medium · CPC title
neutron-gamma activation analysis · CPC title
flaws, defects · CPC title
gamma · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.