Method and apparatus for the determination of electron density in a part volume of a body
First Claim
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1. A method for the determination of the electron density of desired small volumes, called the measuring volume, of a body comprising the steps of directing a first beam of ionizing radiation through said measuring volume to penetrate said volume in a first direction, said first beam having an intensity IO ;
- measuring extra-corporally the intensity of the primary radiation and the intensity of scattered radiation in a second direction of the radiation of said first beam transmitted through said volume, said second direction forming an angle φ
to said first direction;
directing a second beam of ionizing radiation substantially of said intensity IO through said volume in said second direction;
measuring extra-corporally the intensity of the primary radiation and the scattered radiation in said first direction of the radiation of said second beam transmitted through said volume in said second direction, employing such high energy radiation that the Compton effect will be the wholly dominant absorption phenomenon in said volume and in the radiation paths in said first and second direction, and that the change in the absorption cross-section from primary to secondary radiation caused by the Compton shift will be substantial; and
employing the values of said measured intensities to calculate the electron density of said measuring volume in accordance with the formula;
##EQU30## where n = electron densityK = a calibration constantμ
1 = the total linear attenuation coefficient for primary radiationμ
2 = the total linear attenuation coefficient for Compton radiation "forwards"μ
3 = the total linear attenuation coefficient for compton radiation "backwards"Ao = arbitrary expression for the power of the radiation sourceCc = measure of Compton radiationCd = measure of Compton radiationT1 = measure of Transmitted RadiationT2 = measure of Transmitted Radiation.
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Abstract
A method of and an apparatus for the determination of the electron density of small volumes of a body. Two narrow beams of ionizing radiation of substantially equal intensity are subsequently directed through the small volume in two different directions. The intensity of the transmitted radiation as well as the scattered radiation along said two directions is measured extra-corporally, which measurements are employed in computing the electron density of the small volume. The employed radiation is of such high energy that the Compton effect will be the wholly dominant absorption phenomenon in the volume as well as in the radiation paths in the two mentioned directions, and that the change in the absorption cross-section from primary to secondary radiation caused by the Compton shift will be substantial.
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Citations
9 Claims
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1. A method for the determination of the electron density of desired small volumes, called the measuring volume, of a body comprising the steps of directing a first beam of ionizing radiation through said measuring volume to penetrate said volume in a first direction, said first beam having an intensity IO ;
- measuring extra-corporally the intensity of the primary radiation and the intensity of scattered radiation in a second direction of the radiation of said first beam transmitted through said volume, said second direction forming an angle φ
to said first direction;
directing a second beam of ionizing radiation substantially of said intensity IO through said volume in said second direction;
measuring extra-corporally the intensity of the primary radiation and the scattered radiation in said first direction of the radiation of said second beam transmitted through said volume in said second direction, employing such high energy radiation that the Compton effect will be the wholly dominant absorption phenomenon in said volume and in the radiation paths in said first and second direction, and that the change in the absorption cross-section from primary to secondary radiation caused by the Compton shift will be substantial; and
employing the values of said measured intensities to calculate the electron density of said measuring volume in accordance with the formula;
##EQU30## where n = electron densityK = a calibration constant μ
1 = the total linear attenuation coefficient for primary radiationμ
2 = the total linear attenuation coefficient for Compton radiation "forwards"μ
3 = the total linear attenuation coefficient for compton radiation "backwards"Ao = arbitrary expression for the power of the radiation source Cc = measure of Compton radiation Cd = measure of Compton radiation T1 = measure of Transmitted Radiation T2 = measure of Transmitted Radiation. - View Dependent Claims (2, 3, 4, 5)
- measuring extra-corporally the intensity of the primary radiation and the intensity of scattered radiation in a second direction of the radiation of said first beam transmitted through said volume, said second direction forming an angle φ
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6. An apparatus for the determination of the electron density of desired small volumes, called the measuring volume, of a body, the apparatus comprising a first and second radiation source for the successive emission of a first and a second beam of ionizing radiation directed towards a partial volume to be examined, the measuring volume, which first and second beams together form a certain angle φ
- , means for alternately screening said first and second radiation source, a first detector placed diametrically opposite the first radiation source with respect to the measuring volume for measuring the intensity of the transmitted primary radiation from said first radiation source, a second detector placed in the radiation path of said second radiation source for measuring the intensity of said secondary radiation originating from said first primary radiation transmission through said measuring volume, as well as a third detector placed in the radiation path of said first radiation beam for measuring the intensity of said secondary radiation originating from said second primary radiation transmission through the measuring volume, and a fourth detector for measuring the intensity of the transmitted primary radiation from the second radiation source;
means for registering the measured values, said apparatus further comprising means for producing a radiation of such high energy that the Compton effect will be the wholly dominant absorption phenomenon in the measuring volume and in the primary and secondary radiation paths, and that the change in the absorption cross-section from primary to secondary radiation caused by the Compton shift will be substantial. - View Dependent Claims (7, 8, 9)
- , means for alternately screening said first and second radiation source, a first detector placed diametrically opposite the first radiation source with respect to the measuring volume for measuring the intensity of the transmitted primary radiation from said first radiation source, a second detector placed in the radiation path of said second radiation source for measuring the intensity of said secondary radiation originating from said first primary radiation transmission through said measuring volume, as well as a third detector placed in the radiation path of said first radiation beam for measuring the intensity of said secondary radiation originating from said second primary radiation transmission through the measuring volume, and a fourth detector for measuring the intensity of the transmitted primary radiation from the second radiation source;
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Current AssigneeIb Leunbach
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Original AssigneeIb Leunbach
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InventorsLeunbach, Ib
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Primary Examiner(s)Willis, Davis L.
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Application NumberUS05/509,514Time in Patent Office614 DaysField of Search250/272, 250/273, 250/312, 250/361, 250/362, 250/363, 250/366, 250/369, 250/445 T, 250/313, 250/358, 250/306, 250/307US Class Current378/90CPC Class CodesG01N 23/02 by transmitting the radiati...
