Method of measurement of x-ray energy

• US 4,788,706 A
• Filed: 12/17/1987
• Issued: 11/29/1988
• Est. Priority Date: 12/17/1987
• Status: Expired due to Fees

• Current Assignee: General Electric Company
• Original Assignee: General Electric Company
• Inventors: Jacobson, Donald R.
• Primary Examiner(s): Fields, Carolyn E.
• Assistant Examiner(s): NOT, DEFINED
• Application Number:
  US07/134,311
• Time in Patent Office: 348 Days
• Field of Search: 378/4, 378/5, 378/18, 378/207, 250/252.1, 250/358.1
• US Class Current: 378/207
• CPC Class Codes: A61B 6/482 involving multiple energy imaging
• CPC Class Codes: A61B 6/583 using calibration phantoms
• CPC Class Codes: G01N 23/02 by transmitting the radiation through the material
• CPC Class Codes: G01N 33/02 Food
• CPC Class Codes: G01T 1/161 Applications in the field of nuclear medicine, e.g. in vivo counting apparatus for radiation diagnosis A61B6/00

Abstract

X-ray energy in an x-ray beam is determined from a comparison of apparent absorption of energy by three different materials. Initially, the attenuation coefficients of each of the materials as a function of x-ray energy is determined. The ratios of attenuation coefficient differences between two of the materials and between one of the two materials and the third material are plotted over an energy range of interest. Thereafter, the materials are x-rayed and their absorption characteristics determined. The ratio between the differences in absorption characteristics is then calculated in the same manner as the ratio of attenuation coefficients. Matching ratios are then used to identify the energy level of the x-ray beam.

Claims

1. A method for determining the effective energy of an x-ray beam at a predetermined spatial location comprising the steps of:

providing an x-ray target incorporating a first and a second material having x-ray attenuation coefficients μ

₁ and μ

₂, respectively, which vary substantially similarly with variations in x-ray energy and a third material having an attenuation coefficient μ

₃ which varies at a faster rate than said first and said second materials as a function of x-ray energy;

3. The method of claim 1 wherein the step of exposing the target to an x-ray beam comprises the steps of:

scanning the target with a collimated x-ray beam; and

detecting x-rays passing through the target in a plurality of directions within a predetermined plane through the target.

5. The method of claim 1 wherein the step of providing an x-ray target includes the step of positioning each of said first, second and third materials in distinct, symmetrical positions within an x-ray phantom target.

6. The method of claim 1 wherein the step of providing an x-ray target includes the steps of successively positioning each of the three materials in a predetermined location within an x-ray phantom target and separately exposing each material to the x-ray beam.

2. determining the attenuation coefficients of each of the first, second, and third materials over a range of known x-ray energy values;

computing the ratio (μ

₁ -μ

₃)/(μ

₁ -μ

₂) for a plurality of energy levels within a selected x-ray energy band;

exposing the x-ray target to an x-ray beam of an unknown energy;

determining a numerical value representative of x-ray attenuation for each of the first, second, and third materials in the x-ray target;

calculating a ratio corresponding to a difference in numerical values of attenuation between said first and said second materials and a difference in numerical values of attenuation between one of said first and said second materials and the third material;

identifying one of the ratios (μ

₁ -μ

₃)/(μ

₁ -μ

₂) computed for a plurality of energy level having a value substantially equal to the calculated ratio of numerical values of attenuation; and

determining from the identified one of the ratios (μ

₁ -μ

₃)/(μ

₁ -μ

₂) the effective energy level of the x-ray beam.

4. The method of claim 2 wherein the step of determining numerical value comprises the step of:

measuring the x-ray attenuation from the step of detecting for each of the directions relative to all other directions; and

constructing a cross-sectional image giving a relative numerical value for the attenuation of each material in the scan.

7. A method for measuring x-ray energy in a computed tomography (CT) system comprising the steps of:

providing a CT target using first, second, and third materials having predetermined x-ray attenuation coefficients, said first and second materials having similar attenuation variation as a function of x-ray energy over a predetermined range of energy, said third material having an attenuation characteristic which varies between that of said first and said second materials over the predetermined range;

computing ratios of attenuation differences from the difference in attenuation between said first and said second materials at a plurality of selected energies within the predetermined range of energy and the difference in attenuation between one of said first and said second materials and said third material at each of the selected energies;

exposing the target to x-rays in a CT machine and obtaining therefrom CT numbers for each of said first, second, and third materials;

calculating a ratio of the difference between the CT numbers for said first and said second of the materials and the difference between the CT numbers of one of said first and said second materials and the CT number of said third material;

identifying the ratio of the attenuation differences corresponding to the CT ratio; and

identifying a corresponding x-ray energy from the identified ratio.