Method of imaging the atomic number of a sample

• US 4,571,491 A
• Filed: 12/29/1983
• Issued: 02/18/1986
• Est. Priority Date: 12/29/1983
• Status: Expired due to Term

• Current Assignee: Shell Oil Company (Shell Plc)
• Original Assignee: Shell Oil Company (Shell Plc)
• Inventors: Vinegar, Harold J., Wellington, Scott L.
• Primary Examiner(s): Howell, Janice A.
• Application Number:
  US06/566,618
• Time in Patent Office: 782 Days
• Field of Search: 378/5, 378/99, 378/100, 378/207, 250/255, 250/252.1
• US Class Current: 250/252.1
• CPC Class Codes: G01N 23/083 the radiation being X-rays

Abstract

A method of obtaining an atomic number image of an unknown material. A plurality of calibration materials which have a plurality of different known atomic numbers and densities are scanned with a CAT at first and second energies to determine the attenuation coefficients for the plurality of calibration materials at these energies. The energy-dependent coefficients at the first and second energies are determined from the attenuation coefficients for the plurality of calibration materials at the first and second energies according to a predetermined relation. The unknown material is scanned with a CAT at the first and second energies to determine the attenuation coefficients at a plurality of points in a cross section of the unknown material at these energies. The determined energy-dependent coefficients and the determined attenuation coefficients for the unknown material at the first and second energies are used to determine an atomic number image for the unknown material.

Claims

1. A method of obtaining an atomic number image of an unknown material, said method comprising the steps of:

scanning a plurality of calibration materials with a computerized axial tomographic scanner (CAT) at a first energy, said plurality of calibration materials having a plurality of different known atomic numbers, Z_i, and densities, ρ

_i ;

scanning said plurality of calibration materials with a CAT at a second energy;

determining from attenuation coefficients from reconstructed images of said plurality of calibration materials at said first and second energies two energy-dependent coefficients, a and b, at said first and second energies according to the following equation

space="preserve" listing-type="equation">μ

.sub.i =aZ.sup.m.sub.i ρ

.sub.i +bρ

.sub.i

where

μ

_i ;

attenuation coefficient for the i^th calibration material

a;

energy-dependent coefficient

Z_i ;

atomic number for the i^th calibration material

m;

constant in the range of 3.0-4.0

ρ

_i ;

electron density for the i^th calibration material

b;

energy-dependent coefficient; and

scanning said unknown material with a CAT at said first energy;

scanning said unknown material with a CAT at said second energy; and

using said two determined energy coefficients and attenuation coefficients from reconstructed images for said unknown material at said first and second energies to determine an atomic number image of said unknown material.

2. A method as recited in claim 1, wherein said steps of scanning said plurality of calibration materials and said unknown material with a CAT at said first energy comprise scanning said plurality of calibration materials and said unknown material with a CAT at a mean energy in the range from about 80 kiloelectronvolts to about 1 megaelectronvolt and said steps of scanning said plurality of calibration materials and said unknown material at said second energy comprise scanning said plurality of calibration materials and said unknown material with a CAT at a mean energy that is less than 80 kiloelectronvolts.

3. A method as recited in claim 2, wherein said step of determining said two energy-dependent coefficients at said first and second energies comprises determining the energy-dependent coefficients at said first and second energies according to said equation where m is equal to 3.0.

4. A method as recited in claim 6, where said step of using said two determined energy coefficients and attenuation coefficients for said unknown material at said first and second energies to determine an atomic number image of said unknown material comprises determining said atomic number image according to the following equation for each of the plurality of points in the atomic number image cross section ##EQU4## where Z_x *:

effective atomic number for said unknown material

m;

constant equal to 3.0

a₁ ;

determined energy coefficient at said first energy

a₂ ;

determined energy coefficient at said second energy

b₁ ;

determined energy coefficient at said first energy

b₂ ;

determined energy coefficient at said second energy

μ

_1x ;

attenuation coefficient for said unknown material at said first energy

μ

_2x ;

attenuation coefficient for said unknown material at said second energy.

5. A method as recited in claim 4, wherein said unknown material comprises a core sample from a borehole.

6. A method as recited in claim 1, wherein said step of determining said two energy-dependent coefficients at said first and second energies comprises determining the energy-dependent coefficients at said first and second energies according to said equation where m is equal to 3.0.

7. A method as recited in claim 6, wherein said step of using said two determined energy coefficients and attenuation coefficients for said unknown material at said first and second energies to determine an atomic number image of said unknown material comprises determining said atomic number image according to the following equation for each of the plurality of points in the atomic number image cross section ##EQU5## where X_x *:

effective atomic number for said unknown material

m;

constant equal to 3.0

a₁ ;

determined energy coefficient at said first energy

a₂ ;

determined energy coefficient at said second energy

b₁ ;

determined energy coefficient at said first energy

b₂ ;

determined energy coefficient at said second energy

μ

_1x ;

attenuation coefficient for said unknown material at said first energy

μ

_2x ;

attenuation coefficient for said unknown material at said second energy.

8. A method as recited in claim 7, wherein said unknown material comprises a core sample from a borehole.

9. A method as recited in claim 1, wherein said step of using said two determined energy coefficients and attenuation coefficients for said unknown material at said first and second energies to determine an atomic number image of said unknown material comprises determining said atomic number image according to the following equation for each of the plurality of points in the atomic number image cross section ##EQU6## where Z_x *:

effective atomic number for said unknown material

m;

constant in the range of 3.0-4.0

a₁ ;

determined energy coefficient at said first energy

a₂ ;

determined energy coefficient at said second energy

b₁ ;

determined energy coefficient at said first energy

b₂ ;

determined energy coefficient at said second energy

μ

_1x ;

attenuation coefficient for said unknown material at said first energy

μ

_2x ;

attenuation coefficient for said unknown material at said second energy.

10. A method as recited in claim 1, wherein said unknown material comprises a core sample from a borehole.

11. A method as recited in claim 1, wherein said determining said two energy-dependent coefficients employs linear regression techniques.

12. A method of obtaining a density image of an unknown material that is corrected for the effects of atomic composition of said unknown material, said method comprising the steps of:

scanning a plurality of calibration materials with a computerized axial tomographic scanner (CAT) at a first energy, said plurality of calibration materials having a plurality of different known atomic numbers, Z_i, and densities, ρ

_i ;

scanning said plurality of calibration materials with a CAT at a second energy;

determining from attenuation coefficients from reconstructed images of said plurality of calibration materials at said first and second energies two energy-dependent coefficients, a and b, at said first and second energies according to the following equation

space="preserve" listing-type="equation">μ

.sub.i =aZ.sup.m.sub.i ρ

.sub.i +bρ

.sub.i

where

μ

_i ;

attenuation coefficient for the i^th calibration material

a;

energy-dependent coefficient

Z_i ;

atomic number for the i^th calibration material

m;

constant in the range of 3.0-4.0

ρ

_i ;

electron density of the i^th calibration material

b;

energy-dependent coefficient; and

scanning said unknown material with a CAT at said first energy;

scanning said unknown material with a CAT at said second energy; and

using said two determined energy coefficients and attenuation coefficients from reconstructed images for said unknown material at said first and second energies to determine a density image of said unknown material.

13. A method as recited in claim 12, wherein said steps of scanning said plurality of calibration materials and said unknown material with a CAT at said first energy comprise scanning said plurality of calibration materials and said unknown material with a CAT at a mean energy in the range from about 80 kiloelectronvolts to about 1 megaelectronvolt and said steps of scanning said plurality of calibration materials and said unknown material at said second energy comprise scanning said plurality of calibration materials and said unknown material with a CAT at a mean energy that is less than 80 kiloelectronvolts.

14. A method as recited in claim 13, wherein said step of determining said two energy-dependent coefficients at said first and second energies comprises determining the energy-dependent coefficients at said first and second energies according to said equation where m is equal to 3.0.

15. A method as recited in claim 14, wherein said step of using said two determined energy coefficients and attenuation coefficients for said unknown material at said first and second energies to determine a corrected density image of said unknown material comprises determining said density image according to the following equation for each of the plurality of points in the density image cross section ##EQU7## where ρ

_x ;

corrected density for said unknown material

a₁ ;

determined energy coefficient at said first energy

a₂ ;

determined energy coefficient at said second energy

b₁ ;

determined energy coefficient at said first energy

b₂ ;

determined energy coefficient at said second energy

μ

_1x ;

attenuation coefficient for said unknown material at said first energy

μ

_2x ;

attenuation coefficient for said unknown material at said second energy.

16. A method as recited in claim 15, wherein said unknown material comprises a core sample from a borehole.

17. A method as recited in claim 12, wherein said step of determining said two energy-dependent coefficients at said first and second energies comprises determining the energy-dependent coefficients at said first and second energies according to a said equation where m is equal to 3.0.

18. A method as recited in claim 17, wherein said step of using said two determined energy coefficients and attenuation coefficients for said unknown material at said first and second energies to determine a corrected density image of said unknown material comprises determining said density image according to the following equation for each of the plurality of points in the density image cross section ##EQU8## where ρ

_x ;

corrected density for said unknown material

a₁ ;

determined energy coefficient at said first energy

a₂ ;

determined energy coefficient at said second energy

b₁ ;

determined energy coefficient at said first energy

b₂ ;

determined energy coefficient at said second energy

μ

_1x ;

attenuation coefficient for said unknown material at said first energy

μ

_2x ;

attenuation coefficient for said unknown material at said second energy.

19. A method as recited in claim 18, wherein said unknown material comprises a core sample from a borehole.

20. A method as recited in claim 12, wherein said step of using said two determined energy coefficients and attenuation coefficients for said unknown material at said first and second energies to determine a corrected density image of said unknown material comprises determining said density image according to the following equation for each of the plurality of points in the density image cross section ##EQU9## where ρ

_x ;

corrected density for said unknown material

a₁ ;

determined energy coefficient at said first energy

a₂ ;

determined energy coefficient at said second energy

b₁ ;

determined energy coefficient at said first energy

b₂ ;

determined energy coefficient at said second energy

μ

_1x ;

attenuation coefficient for said unknown material at said first energy

μ

_2x ;

attenuation coefficient for said unknown material at said second energy.

21. A method as recited in claim 12, wherein said unknown material comprises a core sample from a borehole.

22. A method as recited in claim 12, wherein said determining said two energy-dependent coefficients employs linear regression techniques.

23. A method of obtaining an atomic number image of an unknown material, comprising:

scanning a plurality of calibration materials having known different atomic numbers, Z_i, and densities, ρ

_i, and said unknown material at a first energy with a computerized axial tomograph (CAT) scanner,

scanning said plurality of calibration materials and said unknown material at a second energy with said CAT scanner,

calculating two energy-dependent coefficients from attenuation coefficients of said calibration materials obtained from reconstructed images of said calibration materials at said first and second energies, and

calculating an effective atomic number image for said unknown material from attenuation coefficients for said unknown material obtained from reconstructed images of said unknown material and said energy-dependent coefficients at said first and second energies.

24. A method of obtaining a density image of an unknown material, comprising;

scanning a plurality of calibration materials having known different atomic numbers, Z_i, and densities, ρ

_i, and said unknown material at a first energy with a computerized axial tomograph (CAT) scanner,

scanning said plurality of calibration materials and said unknown material at a second energy with said CAT scanner,

calculating two energy-dependent coefficients from attenuation coefficients of said calibration materials obtained from reconstructed images of said calibration materials at said first and second energies, and

calculating a density image for said unknown material from attenuation coefficients for said unknown material obtained from reconstructed images of said unknown material and said energy-dependent coefficients at said first and second energies.