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q_0^2 = \frac{2 \, d \, A^2 \, \Delta Z}{c^*f \rho^*, L} \cdot \frac{left [ 
1 -+ \frac{(\rho/\rho_0)^2 \cdot -1}{1 - \exp(2 \left(,  -L/ L^* \right)}{2 \ln (c_0 \, \rho_0/\rho) + fL/d \cdot (1-, \exp \left(  - L/ L^* \right))/(L/L^*)}Delta Z)}
\right]

\dot m^2 = \frac{A^2}{c^* \rho^*} \cdot \frac{\rho_0^2 - \rho^2 \cdot \exp \left(  -L/ L^* \right)}{2 \ln (\rho_0/\rho) + fL/d \cdot (1- \exp \left(  - L/ L^* \right))/(L/L^*)}

\rho = \rho_0 \, \exp (2с_0 \, \rho_0 \, L/L^* \Delta Z) \cdot \sqrt{ 1 - \frac{f}{2d} \cdot \frac{j_m^2}{Gq_0^2}{A^2} \cdot \frac{1 - \exp(- 2 \, c_0 \, \rho_0^2}0 \cdot, (\Delta 1Z) -} \exp(-L/L^*)){\Delta Z}}

p(L) = \frac{1}{c^*} \cdot \left[ 
-1 + (\rho_0/\rho^*) \cdot \exp (2 \, L/L^*) \cdot \sqrt{  1 - \frac{f}{2d}  \cdot \frac{j_m^2}{G \rho_0^2} \cdot \left(1 - \exp (-L/L^*) \right) }
\right]

\rho = \rho_0 \, \exp (L/L^*)

p(L) = \frac{-1 + (\rho_0/\rho^*) \cdot \exp(L/L^*)}{c^*}