Self-compensating X-ray or .gamma.-ray thickness gauge

• US 4,047,029 A
• Filed: 07/02/1976
• Issued: 09/06/1977
• Est. Priority Date: 07/02/1976
• Status: Expired due to Term

• Current Assignee: John J. Allport
• Original Assignee: John J. Allport
• Inventors: Allport, John J.
• Primary Examiner(s): Willis, Davis L.
• Application Number:
  US05/702,285
• Time in Patent Office: 431 Days
• Field of Search: 250/272, 250/273, 250/274, 250/277, 250/278, 250/279, 250/358 R, 250/359, 250/360, 250/308
• US Class Current: 378/90
• CPC Class Codes: G01N 23/083 the radiation being X-rays
• CPC Class Codes: G01N 23/16 the material being a moving sheet or film

Abstract

A gauge for determining the mass per unit area, or alternatively the thickness of sheet material by measuring the attenuation, as well as backscatter, of an X-ray beam or the like, while continuously taking into account deviations and changes in localized material composition, insofar as these have an effect on the transmission coefficient of the beam. Electrical signals representing these deviations are combined with calibration data for given material nominal properties, i.e., nominal composition. The resultant and output signal represents the mass per unit area or thickness.

Claims

1. A system for continuously measuring the mass per unit area of sheet material, whose composition is slightly variable from nominal comprising,

radiation generating means for generating a radiation beam directed into said sheet, said radiation having energy such that a first portion of said beam penetrates said sheet in a straight line from said generating means and a second portion of said beam is scattered from said sheet,

first detector means positioned on the opposite side of said sheet from said radiation generating means in a position to intercept said first portion of said beam for measuring the intensity of said first portion of said beam, and having a first output signal representative of beam intensity transmitted through said sheet material,

second detector means disposed in a position to intercept part of said second beam portion for measuring the intensity of said part and having a second output signal representative of beam intensity scattered from said sheet material,

computing means connected to said first and second detector means for continuously computing the transmission ratio, R₁, by dividing said first output signal by the signal output of said first detector means in the absence of sheet material and computing the scattering ratio, R₂, by dividing said second output signal by the signal output of said second detector means in the presence of very thick standard sheet material, said transmission and scattering ratios, R₁ and R₂ being represented by electrical signals, said computing means including reference means for receiving inputs of nominal material composition and for having stored calibration data therein with respect to said material composition and further having as inputs said signals representative of said transmission ratio, R₁, and said scattering ratio, R₂, said computing means using said ratios R₁ and R₂ with said calibration data and having as an output a corrected absorption coefficient signal μ

_c, said reference means having circuit means interacting with said computing means for receiving said absorption coefficient signal μ

_c, and said transmission ratio signal R₁ for generating a material mass per unit area signal, ρ

T, and an output means for delivering said mass per unit area signal.

2. The system of claim 1 wherein said reference means being operatively connected in said computing means by circuit means for presenting as electrical signals absorption coefficients, μ

₃ and μ

₄, for transmitted and scattered radiation for very massive and thick materials, said connected computing means generating respective polynomials, F(R₁) and G(R₁), and associated electrical signals to be multiplied by respective absorption coefficients of very massive and thick materials, μ

₃ and μ

₄, respectively, for defining signals representing nominal absorption coefficients for radiation transmitted and scattered by the material under test.

3. The system of claim 2 wherein said polynomials are electrically specified in said random access memory by specification of a nominal material for said sheet material.

4. The system of claim 3 wherein said computing means generates a factor A, dependent on the transmission ratio R₁, by means of the equation ##EQU12## and an electrical signal proportional thereto.

5. The system of claim 4 wherein said computing means has as inputs electrical signals representing A, R₁, R₂, and μ

_4r where R₁ is the transmission ratio signal, R₂ is the scattering ratio signal, and μ

_4r is an asymptotic value of the apparent absorption coefficient signal for scattered radiation from very massive and thick standard material, said computing means having circuit means for generating a signal representing the corrected absorption coefficient for scattered radiation, μ

'"'"'₄, for a very massive and thick sheet of material of the same composition as that being measured.

6. The system of claim 5 wherein said signal representing μ

'"'"'₄ is generated by electrical combination of signals for A₁, R₁, R₂ and μ

_4r in accord with the equation ##EQU13##

7. The system of claim 6 wherein said computing means has as inputs electrical signals representing μ

'"'"'₄, μ

₄, μ

₃, F(R₁), said computing means having circuit means for generating a signal representing the corrected absorption coefficient μ

_c for radiation transmitted through the material.

8. The system of claim 7 wherein said computing means has as inputs electrical signals representing the corrected absorption coefficient, μ

_c, and transmission ratio R₁, said computing means having circuit means for generating a signal representing mass per unit area of said sheet material.

9. The system of claim 8 wherein said computing means has as inputs electrical signals representing the mass per unit area of said sheet material and the known density of said sheet material, said computing means having circuit means for generating a signal representing thickness of said sheet material.

10. The apparatus of claim 1 wherein said radiation generating means is an X-ray source.

11. The apparatus of claim 1 wherein said radiation generating means is a gamma ray source.

12. A method for continuously measuring mass per unit area of sheet material whose composition is slightly variable in comparison to nominal material comprising,

generating a beam of penetrating radiation,

measuring the intensity of said beam of penetrating radiation,

directing said beam of penetrating radiation into a sheet material,

measuring the intensity of said radiation transmitted through said sheet material,

measuring the intensity of said radiation scattered by said material,

dividing said measured transmitted intensity by said measured beam intensity to form a beam transmission ratio,

dividing said measured scattered intensity by the scattered intensity expected from a very massive and thick standard material to form a beam scattering ratio,

comparing said beam scattering ratio with another scattering ratio expected from a nominal material at said transmission ratio,

calculating for said sheet material a corrected material absoption coefficient for transmission of penetrating radiation using said scattering ratio comparison, and

calculating the mass per unit area of said sheet material using said transmission ratio and said corrected absorption coefficient.

13. The method of claim 12 further defined by continuously dividing the calculated mass per unit area of said sheet material by the known density of said material thereby yielding the thickness of sheet material whose composition is slightly variable in comparison to material of nominal composition.

14. The method of claim 12 wherein said penetrating radiation is X-ray radiation.

15. The method of claim 12 wherein said penetrating radiation is Gamma radiation.

16. The method of claim 12 wherein said scattered radiation is backscattered from said sheet material.