Difference between revisions of "S coefficient (radiation weighted)"
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</math> | </math> | ||
− | where <math>E_{R,i}</math> is the energy in joules of the i<sup>th</sup> radiation of type <math>R</math> emitted in nuclear transformations of the radionuclide (J); <math>Y_{R,i}</math> is the yield of the i<sup>th</sup> radiation of type <math>R</math> per nuclear transformation [(Bq | + | where <math>E_{R,i}</math> is the energy in joules of the i<sup>th</sup> radiation of type <math>R</math> emitted in nuclear transformations of the radionuclide (J); <math>Y_{R,i}</math> is the yield of the i<sup>th</sup> radiation of type <math>R</math> per nuclear transformation [(Bq s)<sup>-1</sup>]; <math>w_R</math> is the radiation weighting factor for radiation type <math>R</math>; and <math>\phi (r_T \leftarrow r_s, E_{R,i})</math> is the specific absorbed fraction defined as the fraction of energy <math>E_{R,i}</math> of radiation type <math>R</math> emitted within the source region <math>r_S</math> that is absorbed per mass in the target region <math>r_T</math> (kg<sup>-1</sup>). |
[[ICRP Publication 130]], 2015 | [[ICRP Publication 130]], 2015 |
Revision as of 18:55, 19 August 2021
The equivalent dose to target region r_T per nuclear transformation of a given radionuclide in source region r_S, Sv (Bq s)-1.
where E_{R,i} is the energy in joules of the ith radiation of type R emitted in nuclear transformations of the radionuclide (J); Y_{R,i} is the yield of the ith radiation of type R per nuclear transformation [(Bq s)-1]; w_R is the radiation weighting factor for radiation type R; and \phi (r_T \leftarrow r_s, E_{R,i}) is the specific absorbed fraction defined as the fraction of energy E_{R,i} of radiation type R emitted within the source region r_S that is absorbed per mass in the target region r_T (kg-1).
ICRP Publication 130, 2015
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