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Plutonium Biokinetics in Human Body A. Luciani - Kit-Bibliothek - FZK

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3.1.1 MATHEMATICAL TOOLS<br />

3.1.1.1 Solution of a compartmental model<br />

83<br />

3.1 BIOKINETIC MODELLING<br />

As briefly <strong>in</strong>troduced <strong>in</strong> paragraph 1.3.2, the biok<strong>in</strong>etic models used <strong>in</strong> <strong>in</strong>ternal<br />

dosimetry are based on systems of compartments describ<strong>in</strong>g the k<strong>in</strong>etic of the radionuclide of<br />

<strong>in</strong>terest <strong>in</strong> different organs or tissues. The amount of activity <strong>in</strong> the compartments is<br />

calculated by solv<strong>in</strong>g the system of differential equations which mathematically describes the<br />

compartmental model [56]. In case of a s<strong>in</strong>gle acute <strong>in</strong>take the result<strong>in</strong>g system of differential<br />

equations with its <strong>in</strong>itial conditions is given by:<br />

where:<br />

qi(t) is the amount of activity <strong>in</strong> the i-th compartment at time t;<br />

ri,j is the transfer rate from j-th to i-th compartment;<br />

λR is the physical decay constant;<br />

i<br />

q0 is the <strong>in</strong>itial activity amount <strong>in</strong> the i-th compartment.<br />

as:<br />

dq1 t<br />

dt<br />

dq2 t<br />

dt<br />

.......<br />

dq i t<br />

dt<br />

.......<br />

dq n t<br />

dt<br />

n<br />

j 2<br />

n,j 2<br />

j 1<br />

n,j i<br />

j 1<br />

r 1,jq j(t)<br />

r 2, jq j (t)<br />

r i,jq j(t)<br />

n 1<br />

rn,j q j (t)<br />

j 2<br />

q 1(t) r j,1<br />

j 2<br />

n,j2<br />

equation 3.1.1<br />

In the more compact matrix form, the same system of differential equations is written<br />

dq(t)<br />

dt<br />

where:<br />

q(t) is the vector of the amount of activity <strong>in</strong> the n compartments at time t;<br />

R is the matrix of the transfer rates;<br />

I is the unit matrix;<br />

q 0 is the vector of <strong>in</strong>itial conditions.<br />

n<br />

q 2(t) r j,2<br />

j 1<br />

n,ji<br />

q i(t) r j,i<br />

j 1<br />

n 1<br />

q n(t) r j,n<br />

j 2<br />

λ Rq 1(t)<br />

λ Rq 2(t)<br />

λ Rq i(t)<br />

λ Rq n(t)<br />

(R λ RI)q(t) q(0) q 0<br />

1<br />

q1(0) q0 2<br />

q2(0) q0 ........<br />

i<br />

qi (0) q0 ......<br />

n<br />

qn(0) q0 equation 3.1.2

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