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

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

\rho = \rho_0 \, \exp (с_0 \, \rho_0 \, \Delta Z) \cdot \sqrt{ 1 - \frac{f}{2d} \cdot \frac{q_0^2}{A^2} \cdot \frac{1 - \exp(- 2 \, c_0 \, \rho_0 \, \Delta Z) } {\Delta Z}}

p(L) = p_0 + \frac{1}{c^*c_0} \cdot, \left[ 
-1 + (\rho_0/\rho^*) \cdot \exp (2 \, L/L^*) \cdot \sqrt{  1 - \frac{f}{2d}  \cdot \frac{j_m^2\rho}{G \rho_0^20} \cdot \left(1 - \exp (-L/L^*) \right) }
-1 \right]

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

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