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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functions, def<strong>in</strong>ed as reta<strong>in</strong>ed and excreted activity per unit activity of <strong>in</strong>take, respectively, are<br />
calculated. On the basis of the measurements the <strong>in</strong>take can be assessed. In case of<br />
environmental monitor<strong>in</strong>g, such as surface or air contam<strong>in</strong>ation measurements, assumptions<br />
on resuspension factor and breath<strong>in</strong>g habits of exposed subject are made to <strong>in</strong>fer a<br />
hypothetical <strong>in</strong>take. The <strong>in</strong>take assessment is strictly related to the scenario of contam<strong>in</strong>ation<br />
such as time of <strong>in</strong>take, compound, path of <strong>in</strong>take, etc.<br />
In the second step a dose coefficient, commonly taken as committed effective dose<br />
(see Annex) per unit activity of <strong>in</strong>take, can be derived on the basis of the biok<strong>in</strong>etic model.<br />
The same biok<strong>in</strong>etic model adopted <strong>in</strong> the phase of <strong>in</strong>take estimation, must be adopted also <strong>in</strong><br />
calculat<strong>in</strong>g dose coefficients.<br />
Multiply<strong>in</strong>g the estimated <strong>in</strong>take by the calculated dose coefficient, the dose is f<strong>in</strong>ally<br />
obta<strong>in</strong>ed.<br />
Biok<strong>in</strong>etic studies have been carried out s<strong>in</strong>ce many years to describe the timedependent<br />
distribution, both after the <strong>in</strong>troduction of a radioactive compound via a specific<br />
pathway, and after the direct uptake <strong>in</strong>to the blood. For this purpose models for the presystemic<br />
and systemic phases of the contam<strong>in</strong>ation were developed, respectively. In <strong>in</strong>ternal<br />
dosimetry the relevant organs and/or tissues are represented by dist<strong>in</strong>ct compartments, and<br />
generally it is assumed that the radionuclide is transported from one compartment to another<br />
at a rate which is proportional to the amount present <strong>in</strong> the feed<strong>in</strong>g compartment. This type of<br />
behaviour is named first order k<strong>in</strong>etics [56]. Compartmental models are a general tool for<br />
modell<strong>in</strong>g the behaviour of material obey<strong>in</strong>g first order k<strong>in</strong>etics, whether radioactive or stable.<br />
For the specific case of radioactive materials, processes of biological transport are<br />
conveniently separated from radioactive decay. Thus biok<strong>in</strong>etic models normally treat<br />
materials as stable and consequently the transfer rates specified <strong>in</strong> the model represent only<br />
the biological transport. The effect of radioactive decay is taken <strong>in</strong>to account separately by<br />
consider<strong>in</strong>g for each compartment an exit pathway with rate equal to the physical decay<br />
constant.<br />
ICRP has developed models for the pre-systemic phase of the contam<strong>in</strong>ation to<br />
represent the behaviour of radionuclides that have entered the human body via <strong>in</strong>halation and<br />
<strong>in</strong>gestion, and also systemic models for the metabolism of the radionuclides after the uptake<br />
<strong>in</strong>to the blood.<br />
The ICRP model for the respiratory tract [57] dist<strong>in</strong>guishes five regions:<br />
• Extrathoracic airways, divided <strong>in</strong> anterior nasal passage (ET1) and posterior nasal-oral<br />
passage (ET2), <strong>in</strong>clud<strong>in</strong>g also pharynx and larynx.<br />
• Thoracic airways divided <strong>in</strong> bronchial (BB), bronchiolar (bb) and alveolar-<strong>in</strong>terstitial (AI)<br />
regions.<br />
Lymphatic tissues (LNET and LNTH) are associated with extrathoracic and thoracic airways,<br />
respectively. Deposition <strong>in</strong> each region of the respiratory tract is determ<strong>in</strong>ed by the aerosol<br />
particle size and breath<strong>in</strong>g parameters. The clearance from the respiratory tract is treated as<br />
two compet<strong>in</strong>g processes: Particle transport (by mucociliary clearance and translocation to<br />
lymph nodes) and absorption to blood. Particle transport is a function of the deposition site <strong>in</strong><br />
the respiratory tract and of particle size. The mechanical transport be<strong>in</strong>g time dependent, most<br />
regions are subdivided <strong>in</strong>to several compartments with different clearance rates. Absorption to<br />
the blood is treated as a function of the deposition site <strong>in</strong> the respiratory tract and of the<br />
physicochemical form of the radionuclide. Specific dissolution rates are normally<br />
recommended. But if no specific <strong>in</strong>formation is available, default absorption parameters are<br />
given for three dissolution types, namely type F (fast), M (moderate) and S (slow). In case of<br />
the <strong>in</strong>halation of vapours, the respiratory tract deposition is material specific. Values are given<br />
20