Plutonium Biokinetics in Human Body A. Luciani - Kit-Bibliothek - FZK
Plutonium Biokinetics in Human Body A. Luciani - Kit-Bibliothek - FZK
Plutonium Biokinetics in Human Body A. Luciani - Kit-Bibliothek - FZK
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Annex<br />
Quantities used <strong>in</strong> Radiological Protection<br />
and Internal Dosimetry<br />
The <strong>in</strong>teraction of the ioniz<strong>in</strong>g radiations with the biological matter determ<strong>in</strong>e a release of<br />
energy that changes the physical characteristics of atoms and molecules and may thus sometimes<br />
damage cells and tissues. When a damage to cells occurs two effects are possible:<br />
1. The cell can get unable to survive or to reproduce;<br />
2. It can be able to live and reproduce but <strong>in</strong> a modified form.<br />
These two different effects of the <strong>in</strong>teraction of ioniz<strong>in</strong>g radiation have important<br />
consequences for the whole organism the cells belong to.<br />
In the first case if the damage has caused a significant loss of cells the relat<strong>in</strong>g tissue will be<br />
likely characterized by a decrease of its own functions. The probability of caus<strong>in</strong>g such harm will<br />
be zero at small doses but will <strong>in</strong>crease quickly above a certa<strong>in</strong> level of dose, called dose threshold.<br />
Above such threshold the severity of the damage too will <strong>in</strong>crease with the dose. This type of effect<br />
due to the ioniz<strong>in</strong>g radiation is currently called “determ<strong>in</strong>istic”.<br />
In the second case the clone produced by the cell, still alive but subdued to modification<br />
ow<strong>in</strong>g to the ioniz<strong>in</strong>g radiation <strong>in</strong>teraction, may show malignant consequences, after a variable<br />
delay called latency period. The probability of a cancer <strong>in</strong>creases with the dose but the severity of<br />
the cancer is not affeted by the level of the dose. This k<strong>in</strong>d of effect is called “stochastic”. It is<br />
currently assumed that the stochastic effect have no dose threshold and that the probability of<br />
occurrence is roughly proportional to the dose, particularly for doses smaller than the dose threshold<br />
for determ<strong>in</strong>istic effect. In the particular case <strong>in</strong> which the damage occurred <strong>in</strong> a cell for the<br />
transmission of the genetic <strong>in</strong>formation, the effect may result <strong>in</strong> defects <strong>in</strong> the progeny of the<br />
exposed persons. This particular type of stochastic effect is called “hereditary”.<br />
The system of radiation protection has the primary goal of prevent<strong>in</strong>g the occurrence of<br />
determ<strong>in</strong>istic effects and of limit<strong>in</strong>g the effect of the stochastic effects to an acceptable level; this<br />
means that professional activities with exposure to ioniz<strong>in</strong>g radiations should not be characterized<br />
by a risk higher than other professional activities currently considered “safe”.<br />
In order to control the exposure to ioniz<strong>in</strong>g radiation quantities have been expressively<br />
designed and developed by ICRP for radiation protection purposes. The quantities were developed<br />
by ICRP s<strong>in</strong>ce different years [58] up to a wide and deep review and update work presented <strong>in</strong> the<br />
Publication 60 [26].<br />
The fundamental quantity <strong>in</strong> radiation protection is the absorbed dose D given by:<br />
D = d<br />
dm<br />
155<br />
equation A.1<br />
where d is the energy of the ioniz<strong>in</strong>g radiations absorbed by the matter of mass dm. The SI<br />
unit for the absorbed dose is J kg -1 and its special name is “gray” (Gy). The absorbed dose is def<strong>in</strong>ed