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| q_0^2 = \frac{A^2}{c^* \rho^*} \cdot \frac{1 - (\rho/\rho_0)^2 \cdot \exp \left( -L/ L^* \right)}{2 \ln (\rho_0/\rho) + fL/d \cdot (1- \exp \left( - L/ L^* \right))/(L/L^*)} |
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| c^* \, \rho^* = c _0 \, \rho_0 |
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| L^* = c^* \, \rho^* \, G |
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| \rho/\rho_0 = \frac{1+ c^* p}{1+ c^* p_0} |
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| \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^*)} |
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| c^* \, \rho^* = c _0 \, \rho_0 |
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| L^* = c^* \, \rho^* \, G |
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| \rho/\rho_0 = \frac{1+ c^* p}{1+ c^* p_0} |
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anchor | static |
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alignment | left |
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| \rho = \rho_0 \, \exp (c^* \rho^* \, G \, L) \cdot \sqrt{ 1 - \frac{f}{2d} \cdot \frac{j_m^2}{G \, \rho_0^2} \cdot ( 1 - \exp(-2 \, c^* \rho^* \, G \, L))} |
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anchor | static |
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alignment | left |
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| p(L) = \frac{1}{c^*} \cdot \left[
-1 + (1+c^* p_0) \cdot \exp (c^* \rho^* \, G \, L) \cdot \sqrt{ 1 - \frac{f}{2d} \cdot \frac{j_m^2}{G \rho_0^2} \cdot \big(1 - \exp (-2 \, c^* \rho^* \, G \, L) \big) }
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Pressure Profile in GC-proxy static fluid column @model | LaTeX Math Inline |
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body | \dot m = 0, \, q_0 = 0 |
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anchor | static |
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alignment | left |
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| \rho = \rho_0 \, \exp (L/L^*) |
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anchor | static |
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alignment | left |
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| p(L) = \frac{-1 + (1+c^* \, p_0) \cdot \exp(c^* \rho^* G \, LL/L^*)}{c^*} |
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See also
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