X-ray determination of the mass distribution in containers

• US 6,192,101 B1
• Filed: 08/19/1998
• Issued: 02/20/2001
• Est. Priority Date: 08/21/1997
• Status: Expired due to Fees

• Current Assignee: American Science and Engineering Incorporated (OSI Systems Incorporated)
• Original Assignee: American Science and Engineering Incorporated (OSI Systems Incorporated)
• Inventors: Grodzins, Lee
• Primary Examiner(s): Church, Craig E.
• Application Number:
  US09/136,541
• Time in Patent Office: 916 Days
• Field of Search: 378/53-57
• US Class Current: 378/55
• CPC Class Codes: G01N 2223/419 computed tomograph
• CPC Class Codes: G01N 23/046 using tomography, e.g. computed tomography [CT]

Abstract

An apparatus and method for measuring, in a non-invasive manner, the individual mass of objects in containers by means of x-ray transmission radiography in which a beam of penetrating radiation is sent through the container and the transmitted intensity for those photons that interact dominantly via the Compton effect are measured. The masses of the objects in the container are measured with respect to the mass of known objects determined in independent or concurrent measurements.

Claims

1. An apparatus for measuring the mass of at least one object having a characteristic mass attenuation factor to penetrating radiation, the mass attenuation factor being a function at least of the energy of the penetrating radiation, the object being characterized by an unknown composition and being disposed within a container, the apparatus comprising:

a. a source of penetrating radiation for generating a beam incident upon the container at a region of incidence;

b. a scanner for causing the region of incidence to traverse a planar projection of the container;

c. at least one detector having an output proportional to the intensity of the penetrating radiation traversing the container at the region of incidence;

d. an energy selection arrangement permitting analysis of penetrating radiation having energies dominated by Compton scattering; and

e. a controller for determining the mass of the at least one object based on the output of the at least one detector, independently of knowledge of the composition of the at least one object.

2. An apparatus according to claim 1, where the at least one detector includes the energy selection arrangement.

3. An apparatus according to claim 1, further comprising a modulator for alternating interposition of a fiducial mass in the beam.

4. An apparatus according to claim 1, wherein the energy selection arrangement permits analysis of penetrating radiation having energies in excess of 60 keV.

5. An apparatus according to claim 1, wherein the beam includes a fan beam.

6. An apparatus according to claim 1, wherein the beam includes a pencil beam.

7. An apparatus according to claim 1, further comprising a fiducial mass for intermittent interposition in the beam for normalizing the output of the at least one detector.

8. A method for measuring the mass of at least one object having a characteristic mass attenuation factor to penetrating radiation, the mass attenuation factor being a function at least of the energy of the penetrating radiation, the object being disposed within a container, the method comprising:

a. generating a beam of penetrating radiation incident upon the container at a region of incidence;

b. scanning the region of incidence such as to traverse a planar projection of the container;

c. selecting a range of energies of penetrating radiation dominated by Compton scattering for detection;

d. detecting the penetrating radiation traversing the container at the selected range of energies at the region of incidence;

e. producing a detector output proportional to the intensity of the penetrating radiation traversing the container; and

f. determining the mass of the at least one object based on the detector output.

9. A method according to claim 8, further comprising the step of storing the detector output in at least one memory array to produce at least one image.

10. A method according to claim 9, further comprising the step of interposing a fiducial mass alternatingly within the beam of penetrating radiation.

11. A method according to claim 9, further comprising the step of discriminating between detected penetrating radiation of energy greater and less than a predetermined discriminant energy.

12. A method according to claim 11, further comprising the step of determining a charateristic atomic number associated with the at least one object.

13. A method according to claim 10, further comprising the step of storing the detector output in at least one memory array to produce at least one image.

14. A method according to claim 13, wherein the step of storing the detector output includes storing the detector output corresponding to an interposed fiducial mass in a first memory array to produce a first image and storing the detector output corresponding to no interposed fiducial mass in a second memory array to produce a second image.