User Tools

Site Tools


laws:wavat

Differences

This shows you the differences between two versions of the page.

Link to this comparison view

Both sides previous revision Previous revision
Next revision
Previous revision
laws:wavat [2019/09/20 14:35]
helene
laws:wavat [2023/12/12 16:47] (current)
gilles [WAVAT/WAVAT2/WAVAT3]
Line 11: Line 11:
  
 === Ecoulement du liquide et de la vapeur === === Ecoulement du liquide et de la vapeur ===
-En partant de l’équation de Darcy, la vitesse du liquide ( Volume de fluide par unité de surface de sol ) est donnée par :+En partant de l’équation de Darcy, la vitesse du liquide (Volume de fluide par unité de surface de sol) est donnée par :
 \[ \[
 \vec{q_l} = - \frac{k_w}{\mu_w}\left[ \vec{grad}(p_w) + g \rho_w \vec{grad}(y)\right]\ \text{où}\ k_w = K_w \frac{\mu_w}{\rho_w g}\left[ m^2\right] \vec{q_l} = - \frac{k_w}{\mu_w}\left[ \vec{grad}(p_w) + g \rho_w \vec{grad}(y)\right]\ \text{où}\ k_w = K_w \frac{\mu_w}{\rho_w g}\left[ m^2\right]
Line 230: Line 230:
 Following empirical formulations for describing the evolution of the relative permeability,​ the thermal conductivity and saturation with the suction are possible: see [[appendices:​a8|Appendix 8]]. Following empirical formulations for describing the evolution of the relative permeability,​ the thermal conductivity and saturation with the suction are possible: see [[appendices:​a8|Appendix 8]].
 For any suction lower than air entry value (AIREV), the saturation is equal to SRFIELD value. \\  For any suction lower than air entry value (AIREV), the saturation is equal to SRFIELD value. \\ 
-__Kozeny Karman formulation :__+__Kozeny Karman formulation:​__
 \[K = C_0 \frac{n^{EXPN}}{(1-n)^{EXPM}}\] \[K = C_0 \frac{n^{EXPN}}{(1-n)^{EXPM}}\]
 $C_0$ is computed automatically from $C_0 = K_0 \frac{(1-n_0)^{EXPM}}{(n_0)^{EXPn}}$ \\ $C_0$ is computed automatically from $C_0 = K_0 \frac{(1-n_0)^{EXPM}}{(n_0)^{EXPn}}$ \\
-__GDR Momas formulation :__+__GDR Momas formulation:​__
 \[ \[
 \frac{k}{k_0} = 1+EXPM\left[ \phi - \phi_0\right]^{EXPN}\ \text{où}\ EXPM = 2.10^{12}\ \text{et}\ EXPN = 3 \frac{k}{k_0} = 1+EXPM\left[ \phi - \phi_0\right]^{EXPN}\ \text{où}\ EXPM = 2.10^{12}\ \text{et}\ EXPN = 3
 \] \]
  
-__Coupling permeability-deformation formulation :__ (only in 2D)+__Coupling permeability-deformation formulation:​__ (only in 2D)
 \[ \[
 K_{ij} = \sum_n K_n^0 (1+A\varepsilon_n^T)^3\beta_{ij} (\alpha_n) K_{ij} = \sum_n K_n^0 (1+A\varepsilon_n^T)^3\beta_{ij} (\alpha_n)
laws/wavat.1568982900.txt.gz · Last modified: 2020/08/25 15:35 (external edit)