Occupational Intakes of Radionuclides Part 1 - ICRP
Occupational Intakes of Radionuclides Part 1 - ICRP
Occupational Intakes of Radionuclides Part 1 - ICRP
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
3381<br />
3382<br />
3383<br />
3384<br />
3385<br />
3386<br />
3387<br />
3388<br />
3389<br />
3390<br />
3391<br />
3392<br />
3393<br />
3394<br />
3395<br />
3396<br />
3397<br />
3398<br />
3399<br />
3400<br />
3401<br />
3402<br />
3403<br />
3404<br />
3405<br />
3406<br />
3407<br />
3408<br />
3409<br />
3410<br />
3411<br />
3412<br />
3413<br />
3414<br />
3415<br />
3416<br />
3417<br />
3418<br />
3419<br />
DRAFT REPORT FOR CONSULTATION<br />
For both sexes the equivalent dose rate H ( rT<br />
, t)<br />
in target tissue rT at time t after an<br />
acute intake is expressed as<br />
<br />
H ( r , t)<br />
A(<br />
r , t)<br />
S ( r r ) (3)<br />
T<br />
r<br />
S<br />
S<br />
where<br />
A( rS<br />
, t)<br />
is the activity, Bq, <strong>of</strong> the radionuclide in source region rS at time t after<br />
intake for the reference male or female; in this report series, only male<br />
values are used;<br />
S w ( rT<br />
rS<br />
) is the radiation-weighted S value (Bolch et al, 2009); i.e. the equivalent<br />
dose in target tissue rT per nuclear transformation in source region rS,<br />
Sv (Bq s) -1 , for the reference male or female.<br />
(232) The first factor in equation (3) is derived with biokinetic models which<br />
describe the uptake <strong>of</strong> activity into the body, its distribution and retention within body<br />
regions, and its excretion from the body. The second factor is derived with dosimetric<br />
models which are used to calculate the dose to target tissues arising from<br />
transformations in source regions.<br />
3.7.1 Dosimetric models<br />
(233) The equivalent dose in target tissue rT per nuclear transformation in source<br />
region rS, is calculated by:<br />
where<br />
E R,<br />
i<br />
Y R,<br />
i<br />
S<br />
w<br />
( r<br />
T<br />
r ) <br />
S<br />
wR <br />
E<br />
R,<br />
i<br />
98<br />
w<br />
Y<br />
R,<br />
i<br />
R i T<br />
T<br />
T<br />
S<br />
(<br />
r r , E<br />
M ( r )<br />
is the energy <strong>of</strong> the i th nuclear transition <strong>of</strong> radiation type R, in Mev,<br />
is the yield <strong>of</strong> i th radiation <strong>of</strong> type R per nuclear transformation, (Bq s) -<br />
1 ,<br />
w R is the radiation weighting factor for radiation type R, Table 1<br />
r r , E ) is the absorbed fraction, defined as the fraction <strong>of</strong> energy ER,i <strong>of</strong><br />
( T S R,i<br />
radiation type R emitted within the source region rS that is absorbed in<br />
the target tissue rT,<br />
M ( rT<br />
) is the mass <strong>of</strong> target tissue rT, kg.<br />
(234) The energies and yields <strong>of</strong> the emitted radiations, E and Y R,<br />
i<br />
R,<br />
i , are taken<br />
from Publication 107 (<strong>ICRP</strong>, 2008), which supersedes Publication 38 (<strong>ICRP</strong>, 1983).<br />
For β radiation and neutrons accompanying spontaneous fission, the spectral data are<br />
used in the calculation <strong>of</strong> Sw rather than mean values. The sex-dependent target tissue<br />
S<br />
R,<br />
i<br />
)<br />
(4)