multilayer cavity ionization chamber
An ionization chamber and cavity technology, applied in circuits, discharge tubes, electrical components, etc., can solve problems such as uncertainty, achieve the effects of accurate measurement, cost savings, and avoid calibration steps
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Embodiment 1
[0022] In this embodiment, the air kerma energy of high-energy photons with an average energy of 6.62 MeV is measured at a reference point of 1 m.
[0023] First, a basic thin-walled ionization chamber is selected, the thickness of the first layer of the chamber wall is 4mm, the material is graphite, and the sensitive volume of the basic unit is 50cm 3 . exist 137 The ionization chamber is calibrated in the Cs reference radiation field, and the ionization chamber is obtained at 137 Calibration factor N in Cs reference radiation field E , according to N E Make the change curve of the ionization current of the ionization chamber with the thickness of the chamber wall, that is, the effective weakening curve, and according to the following formula:
[0024] N D = 1 ρ · v · ( W e ...
Embodiment 2
[0033] The measurement object is the same as that in Embodiment 1, except that the connection mode of the hemispherical chamber wall is screw connection. The measured air kerma is 8.5μGy / h with a relative uncertainty of 3.3%.
[0034] The specific principle of measuring air kerma in the multilayer cavity ionization chamber provided by the present invention is:
[0035] The core formula for the measurement of high-energy photons is shown in Equation 1:
[0036] K a = ( μ tr μ en ) · K a , C . . . ( 1 )
[0037] It can be seen from formula 1 that the air kerma K is obtained by measuring the collision air kerma a,C , w...
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Abstract
Description
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Application Information
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