Prompt gamma neutron activation analysis system

• US 5,539,788 A
• Filed: 10/08/1992
• Issued: 07/23/1996
• Est. Priority Date: 10/08/1992
• Status: Expired due to Term

• Current Assignee: Westinghouse Electric Company LLC (Brookfield Asset Management Incorporated)
• Original Assignee: Westinghouse Electric Company LLC (Brookfield Asset Management Incorporated)
• Inventors: Seidel, John G., Gonzalez, Joseph L., Bartko, John, Congedo, Thomas V., McLaughlin, David F., Lahoda, Edward J., Ruddy, Frank H., Grant, David C.
• Primary Examiner(s): Behrend, Harvey E.
• Application Number:
  US07/958,215
• Time in Patent Office: 1,384 Days
• Field of Search: 376/159, 376/160-166, 250/390.04, 250/390.07, 250/390.12, 250/391, 250/392, 250/253
• US Class Current: 376/159
• CPC Class Codes: G01N 2223/0745 neutron-gamma activation analysis
• CPC Class Codes: G01N 2223/204 source created from radiated target
• CPC Class Codes: G01N 2223/601 density profile
• CPC Class Codes: G01N 23/222 using neutron activation analysis [NAA]
• CPC Class Codes: G01V 5/02 specially adapted for surface logging, e.g. from aircraft

Abstract

A system for determining depth profiles of concentrations of hazardous elements in soils comprises a neutron source for generating neutrons of a first energy level and irradiating a volume of soil with the neutrons. Nuclear reactions are effected within the soil and gamma radiation is emitted from the soil. The system also includes an array of gamma detectors for detecting gamma radiation emitted from the soil; source electronics for controlling the width of regularly repeated pulses of neutrons generated by the neutron source; detector electronics associated with the gamma detectors for amplifying and digitalizing signals generated by the gamma detectors and storing data representing the digitalized signals; spectral analysis software for analyzing the data and determining the concentrations of selected target elements in the soil; and an acquisition interface module (AIM). The AIM controls the timing of the source and detector electronics such that the neutron source generates neutrons in regularly repeated bursts of a prescribed pulse width and the detectors and detector electronics detect gamma rays during a plurality of time intervals associated with the burst and acquire groups of data. Each group is indicative of a number of gamma rays emitted and their energy levels during a corresponding time interval. The system also includes a mobile platform carrying the neutron source, array of gamma ray detectors and software for determining a depth profile of a target element. Trace elements can also be detected with the disclosed system.

Claims

1. A method for analyzing an interrogation volume containing a prescribed target element, comprising the steps of:

(a) irradiating an interrogation volume with a neutron burst characterized by an intensity and pulse width, and thereby effecting an emission of gamma radiation from said interrogation volume;

(b) acquiring groups of gamma radiation data during a plurality of time intervals, each group being indicative of the number or intensity of gamma rays and energy levels of said gamma rays during a corresponding time interval, and a first group corresponding to a first interval during which said neutron burst is on, and at least one other group corresponding to a time interval during which said neutron burst is off; and

(c) analyzing said gamma data to detect the presence and determine the amount of said prescribed target element in said interrogation volume and to determine whether said prescribed target element is present within a prescribed depth range in said interrogation volume; and

(d) determining calibration data by carrying out the following sub-steps;

(1) placing a slug of mass M of said target element at a plurality of depths, including;

0 inches;

X₁, where X₁ is the deepest depth from which gamma rays of energy E₁ can escape the interrogation volume in sufficient numbers to be detected; and

X₂, where X₂ is the deepest depth from which gamma rays of energy E₂ can escape the interrogation volume in sufficient numbers to be detected; and

measuring yields Y_E1 (0), Y_E1 (X₁) of gamma rays of energy E₁ at depths of 0 inches and X₁, respectively, and Y_E2 (0), Y_E2 (X₁), Y_E2 (X₂) of gamma rays of energy E₂ at depths of 0 inches, X₁ and X₂, respectively;

(2) defining the following ratios;

##EQU9## performing a field measurement of yields y(E₁), y(E₂) of gamma rays of energies E₁, E₂, respectively;

performing a depth inference calculation by determining whether y(E₂)/y(E₁) is greater than R₂₁ (X₁) and whether y(E₁) is greater than 0, and then determining a range of depths at which said target element is located by the following formulas;

Case 1

if y(E₂)/y(E₁) is greater than R₂₁ (X₁) and y(E₁) is greater than 0, then the target element is present between 0 and X₁ and between X₁ and X₂ ;

Case 2

if y(E₂)/y(E₁) is less than R₂₁ (X₁) and y(E₁) is greater than 0, then the target element is between 0 and X₁ ;

Case 3

if y(E₂) is greater than 0 and y(E₁) is 0, then the target element is between X₁, and X₂ ; and

then, performing an equivalent mass calculation by the following formulas;

##EQU10## wherein ES_max and ES_min represent the maximum and minimum equivalent mass within the specified ranges;

wherein steps a, b, and c are performed with a neutron source, detector and analysis system, respectively, wherein said neutron source, detector and analysis system are maintained outside said interrogation volume and in a non-contacting relation with said target element.

2. The method recited in claim 1, wherein said pulse width is approximately 100-500 μ

s.

3. The method recited in claim 1, wherein said plurality of time intervals spans approximately 5000 μ

s.

4. The method recited in claim 1, wherein step (a) comprises generating neutrons with energies of approximately 14 MeV.

5. The method recited in claim 1, wherein step (a) comprises generating neutrons with energies of approximately 3 MeV.

6. The method recited in claim 1, wherein step (a) comprises generating neutrons with energies of approximately 0.025 eV.

7. The method recited in claim 1, wherein step (a) comprises generating neutrons with energies of approximately 750 keV.

8. The method recited in claim 1, wherein said analyzing step for determining whether said target element is present within a first prescribed depth range comprises the step of computing a depth at which said neutrons have energy appropriate to initiate a reaction that produces gamma radiation indicative of said target element.

9. The method recited in claim 1, further comprising the step of generating depth profile data representing the amount of said target element at a plurality of depth ranges in said interrogation volume.

10. The method recited in claim 1, wherein said target element is a soil contaminant.

11. The method recited in claim 1, wherein said target element is a member of a group consisting of uranium, thorium, cadmium, and copper.

12. The method recited in claim 1, wherein said target element is a member of a group consisting of Cl, Cu, Cd, Fe, Hg, Ni, Pb, Th, and U.