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US3840746A Expired / Lapsed US ⏱️ 0.0 years remaining

Gamma ray density probe utilizing a pair of gamma ray sources and a gamma ray detector

Assignee: Applied Inventions Corp
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Filing: 1971-12-13
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Granted: 1974-10-08
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Expires: 1991-12-13
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Abstract

Abstract A gamma ray density probe utilizing a pair of gamma ray sources and a gamma ray detection system which measures separately and then builds the ratio of the radiation scattered from each of the two sources.

Inventors

  • 👤 P Kehler

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-10-24 18:06
CPC Classifications
G; G01; G01V; G01V5/00; G01V5/04; G01V5/08; G01V5/12; G01V5/14

Claims Analysis

Total Claims: 8
Claim 1
Independent Claim 424 words
A gamma ray density probe utilizing a first collimated beam of gamma rays, a second collimated beam of gamma rays having the same energy as the gamma rays in said first collimated beam, a collimated gamma ray detector, a beam controlling means, a switching means, a first pulse storing means, a second pulse storing means, a ratio building means and an output means, said first collimated beam of gamma rays being emitted into a sample of unknown density from a first reference plane along at least one trajectory at an incident angle of Alpha with respect to said first reference plane, said second collimated beam of gamma rays being emitted into said sample of unknown density from a second reference plane along at least one trajectory at the same incident angle Alpha with respect to said second reference plane, said collimated gamma ray detector being located in a third reference plane and generating an output pulse whenever detecting gamma rays that are scattered from said first and said second collimated beams of gamma rays under an angle Beta towards said collimated gamma ray detaector and that are incident on said gamma ray detector at an incident angle of ( Beta - Alpha ) with respect to said third reference plane, said third reference plane being unequally spaced from said first reference plane and said second reference plane, said beam controlling means turning off said first collimated beam of gamma rays whenever said second collimated beam of gamma rays is turned on and vice versa, said switching means sensing the position of said beam controlling means and opening said first pulse storing means for storage of pulses from said collimated gamma ray detector whenever said first collimated beam of gamma rays is turned on and opening said second pulse storing means for storage of pulses from said collimated gamma ray detector whenever said second collimated beam of gamma rays is turned on, said ratio building means computing the ratio of the number of pulses stored in said first pulse storing means to the number of pulses stored in said second pulse storing means, said ratio being displayed by said output means and being interpreted in terms of the density of said sample of unknown density being irradiated by said first collimated beam of gamma rays and said second collimated beam of gamma rays, and said interpretation of density of said sample being independent of the presence of uniform layers of interfering materials located between said gamma ray density probe and said sample of unknown density.
Claim 2
Dependent Claim 424 words
A gamma ray density probe utilizing a first collimated beam of gamma rays, a second collimated beam of gamma rays having the same energy as the gamma rays in said first collimated beam, a collimated gamma ray detector, a beam controlling means, a switching means, a first pulse storing means, a second pulse storing means, a ratio building means and an output means, said first collimated beam of gamma rays being emitted into a sample of unknown density from a first reference plane along at least one trajectory at an incident angle of Alpha with respect to said first reference plane, said second collimated beam of gamma rays being emitted into said sample of unknown density from a second reference plane along at least one trajectory at the same incident angle Alpha with respect to said second reference plane, said collimated gamma ray detector being located in a third reference plane and generating an output pulse whenever detecting gamma rays that are scattered from said first and said second collimated beams of gamma rays under an angle Beta towards said collimated gamma ray detaector and that are incident on said gamma ray detector at an incident angle of ( Beta - Alpha ) with respect to said third reference plane, said third reference plane being unequally spaced from said first reference plane and said second reference plane, said beam controlling means turning off said first collimated beam of gamma rays whenever said second collimated beam of gamma rays is turned on and vice versa, said switching means sensing the position of said beam controlling means and opening said first pulse storing means for storage of pulses from said collimated gamma ray detector whenever said first collimated beam of gamma rays is turned on and opening said second pulse storing means for storage of pulses from said collimated gamma ray detector whenever said second collimated beam of gamma rays is turned on, said ratio building means computing the ratio of the number of pulses stored in said first pulse storing means to the number of pulses stored in said second pulse storing means, said ratio being displayed by said output means and being interpreted in terms of the density of said sample of unknown density being irradiated by said first collimated beam of gamma rays and said second collimated beam of gamma rays, and said interpretation of density of said sample being independent of the presence of uniform layers of interfering materials located between said gamma ray density probe and said sample of unknown density.
Claim 3
Dependent Claim 140 words
A gamma ray density probe in accordance with claim 1, and comprising a ratio averaging means, wherein said beam controlling means allows a continuous density measurement by initiating repetitive irradiation cycles, each of said irradiation cycles comprising a first time interval in which said first collimated beam of gamma rays is turned on and a second time interval in which said second collimated beam of gamma rays is turned on, said ratio building device computing for each of said irradiation cycles the ratio of the number of pulses stored in said first pulse storing means to the number of pulses stored in said second pulse storing means, said ratio averaging means having a definite time constant over which it averages the ratios computed by said ratio building device, said definite time constant being longer than one of said irradiation cycles.
Claim 4
Dependent Claim 133 words
A gamma ray density probe in accordance with claim 1, wherein said beam controlling means allows a continuous density measurement by initiating repetitive irradiation cycles, each of said irradiation cycles comprising a first time interval in which said first collimated beam of gamma rays is turned on and a second time interval in which said second collimated beam of gamma rays is turned on, said first and second pulse storing means having definite time constants over which the average rate of received pulses is derived, said definite time constants being longer than one of said irradiation cycles, and said ratio building device computing the ratio of said average rate of received pulses derived by said first pulse storing means to said average rate of received pulses derived by said second pulse storing means.
Claim 5
Dependent Claim 109 words
A gamma ray density probe in accordance with claim 1, wherein said first collimated beam of gamma rays and said second collimated beam of gamma rays are produced by said beam controlling means, by a first gamma ray source that is permanently positioned behind a first collimator and by a second gamma ray source that is permaneNtly positioned behind a second collimator, said beam controlling means being a mechanical shutter that oscillates linearly and interrupts alternately the beam of gamma rays emitted by said first gamma ray source through said first collimator and the beam of gamma rays emitted by said second gamma ray source through said second collimator.
Claim 6
Dependent Claim 156 words
A gamma ray density probe in accordance with claim 1, wherein said first collimated beam of gamma rays and said second collimated beam of gamma rays are produced by said beam controlling means, by a first gamma ray source that is positioned permanently behind a first collimator and by a second gamma ray source that is positioned permanently behind a second collimator, said beam controlling means being a rotary shutter of cylindrical form that surrounds said first gamma ray source, said second gamma ray source, said first collimator and said second collimator, and which has circumferentially segmented slots cut through its wall in such a way that, during rotation of said beam controlling means around said first source and said first collimator and said second source and said second collimator, only said first collimated beam of gamma rays or said second collimated beam of gamma rays are transmitted through said slots in said beam controlling means.
Claim 7
Dependent Claim 92 words
A gamma ray density probe in accordance with claim 1, wherein said first collimated beam of gamma rays and said second collimated beam of gamma rays are produced by said beam controlling means, by a first collimator, by a second collimator and by a gamma ray source, said beam controlling means positioning said gamma ray source behind said first collimator to produce said first collimated beam of gamma rays, and said beam controlling means positioning said gamma ray source behind said second collimator to produce said second collimated beam of gamma rays.
Claim 8
Dependent Claim 73 words
A gamma ray density probe in accordance with claim 1, further comprising a pulse discimination means, wherein said pulse discrimination means passes only those pulses to said first pulse storing means and to said second pulse storing means, that are produced by those gamma rays of said first and second collimated beams of gamma rays that were scattered only once in said sample of unknown density before reaching said collimated gamma ray detector.

References Cited (Backward Citations)

No citation records indexed.

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1977-10-07 1978-04-08 1978-10-08 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 1981-10-07 1982-04-08 1982-10-08 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 1985-10-07 1986-04-08 1986-10-08 $7700.00 Window Closed / Lapsed

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