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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}

Q_{\rm max}=\frac{q_0}{D_0 \cdot (1-b)}

D(t) = D_0 = \rm const

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

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

RPR(t) = \tau_0 + \frac{\tau_0 \, q_0 \, b /}{(1-b)} \, \frac{1}{q(t)}

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