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Table B.25: Red bone marrow in the whole body - Helmholtz ...

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5<br />

3. Calculational method<br />

___________________________________________________________<br />

The organ dose conversion factors were calculated us<strong>in</strong>g a computer code<br />

simulat<strong>in</strong>g photon transport <strong>in</strong> various media. For this procedure, three<br />

ma<strong>in</strong> components are necessary: a model of <strong>the</strong> radiation source, a technique<br />

to simulate <strong>the</strong> radiation <strong>in</strong>teractions and energy depositions and a<br />

model of <strong>the</strong> human <strong>body</strong>.<br />

Accord<strong>in</strong>g to <strong>the</strong> irradiation conditions mentioned above, <strong>the</strong> radiation<br />

source was modelled as a po<strong>in</strong>t source rotat<strong>in</strong>g around <strong>the</strong> longitud<strong>in</strong>al axis<br />

of <strong>the</strong> <strong>body</strong>; <strong>the</strong> beam size at <strong>the</strong> axis of rotation was 1 cm <strong>in</strong> height and<br />

50 cm <strong>in</strong> width for <strong>the</strong> symmetrical beam (for asymmetrical beams, <strong>the</strong><br />

width was reduced on one side). To simulate <strong>the</strong> x ray spectra as <strong>the</strong>y<br />

emerge from <strong>the</strong> x ray tube, a semi-empirical method was used consider<strong>in</strong>g<br />

<strong>the</strong> target material, <strong>in</strong>herent as well as added filtration, air path, target<br />

angle and tube voltage /8/.<br />

3.1. Monte Carlo method<br />

The radiation transport <strong>in</strong> <strong>the</strong> phantoms was calculated us<strong>in</strong>g a Monte<br />

Carlo code follow<strong>in</strong>g <strong>in</strong>dividual photon histories. For each s<strong>in</strong>gle particle<br />

history, <strong>the</strong> parameters <strong>in</strong>fluenc<strong>in</strong>g its actual course are selected randomly<br />

from <strong>the</strong>ir probability distributions. The radiation <strong>in</strong>teraction processes<br />

considered were photoelectric absorption and Compton scatter<strong>in</strong>g. The<br />

cross section data for <strong>the</strong> radiation <strong>in</strong>teractions were taken from <strong>the</strong> Oak<br />

Ridge National Laboratory /9/. The energy was regarded as be<strong>in</strong>g deposited<br />

at <strong>the</strong> po<strong>in</strong>t of photon <strong>in</strong>teraction; secondary particles were not followed<br />

("Kerma approximation"). A more detailed description of <strong>the</strong> photon<br />

transport code used is given elsewhere /10/.<br />

The absorbed doses were obta<strong>in</strong>ed by divid<strong>in</strong>g <strong>the</strong> total amount of energy<br />

deposited <strong>in</strong> an organ by <strong>the</strong> mass of this organ. It is to be emphasised that

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