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Occupational Intakes of Radionuclides Part 1 - ICRP

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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)

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