Différences

Ci-dessous, les différences entre deux révisions de la page.

--- sunfluidh:gravity_namelist [2017/07/03 18:52] – yann
+++ sunfluidh:gravity_namelist [2019/08/01 09:27] (Version actuelle) – yann
@@ Ligne 43: / Ligne 43: @@
 Where $G_0$ is norm of the force of gravity (or the buoyancy force).\\
 \\
-b__**Remarks**__
+__Remarks__
-  The angle ranges are $ -90 \le $ Gravity_Angle_IJ $ \le +90$ and $ 0 \le $ Gravity_Angle_IJ $ \le +180$. \\
+  * The angle ranges are $ -90 \le $ Gravity_Angle_IJ $ \le +90$ and $ 0 \le $ Gravity_Angle_IK $ \le +180$. \\
-  From the definition of angles, note that the vector $\vec{g}$ is oriented along the $-\vec{K}$ axis while Gravity_Angle_IK= 0 and $\vec{g}$ is in the plan IJ while Gravity_Angle_IK= 90.\\
+  * From the definition of angles, note that the vector $\vec{g}$ is oriented along the $-\vec{K}$ axis while Gravity_Angle_IK= 0 and $\vec{g}$ is in the plan IJ while Gravity_Angle_IK= 90.\\
 Following the type of simulation and the choice on the form of equations (dimensional, dimensionless, the scales used in order to define the non-dimensional form of equations, etc ...), the term $G_0$ can be written following different ways. For instance, the buoyancy force can be read as :
@@ Ligne 56: / Ligne 56: @@
 in the momentum equations for incompressible flows under Boussinesq hypothesis. In this case
    * $G_0= \beta.g_0$ where $\beta$ is the thermal expansion coefficient of the fluid considered.
-   * $T_0$ is the reference temperature defined in the namelist [[sunfluidh:fluid_properties_namelist|"Fluid_Properties"]].
+   * $T_0$ is the reference temperature defined in the namelist [[sunfluidh:temperature_initialization_namelist|"Temperature_Initialization"]].
 As a consequence the generalized form of $G_0$ in the code is :
 $$G_0= \beta.g_0$$