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q(t)=q_0 \exp \left( -D_0 \, t \right)

q(t) = \frac{q_0}{ \left( 1+b \cdot D_0 \cdot t \right)^{1/b} }

q(t)=\frac{q_0}{1+D_0 \, t} 

Q(t)=\frac{q_0-q(t)}{D_0}

Q(t)=\frac{q_0}{D_0 \, (1-b)} \, \left[ 1- \left( \frac{q(t)}{q_0} \right)^{1-b}  \right]

Q(t)=\frac{q_0}{D_0} \, \ln \left[ \frac{q_0}{q(t)} \right]

Q_{\rm max}=\frac{q_0}{D_0}

D(t) =\frac{D_0}{1+ b \cdot D_0 \cdot t}

D(t) = \frac{D_0}{1+ D_0 \cdot t}

\tau(t) = \tau_0 = \rm const

\tau(t) = \tau_0 + b \cdot t

\tau(t) = \tau_0 + t

Q_{\rm max}=\frac{q_0}{D_0}RPR(t) = \tau(t) \tau_0 = \rm const

Q_{\rm max}=\frac{q_0}{D_0RPR(t) = \tau_0 + b \cdot (1-b)}t

Q_{RPR(t) = \rm max}=\infty{not applicable due to infinite volume}