From 506a8ef1d0a15552fe9b4b3bb1c070e18bafc374 Mon Sep 17 00:00:00 2001 From: Ann Almgren Date: Wed, 17 Oct 2018 19:36:14 -0700 Subject: [PATCH] Define variables --- docs/source/FluidEquations.rst | 26 ++++++++++++++++++++++---- 1 file changed, 22 insertions(+), 4 deletions(-) diff --git a/docs/source/FluidEquations.rst b/docs/source/FluidEquations.rst index dca9b8d..2ad1374 100644 --- a/docs/source/FluidEquations.rst +++ b/docs/source/FluidEquations.rst @@ -1,6 +1,24 @@ Fluid Equations =============== +We define the following fluid variables: + +:math:`\rho_g = ` fluid density (assumed to be constant in the absence of reactions) + +:math:`\varepsilon_g = ` volume fraction of fluid (accounts only for displacement of fluid by particle, does not account for the EB walls) + +:math:`U_g = ` fluid velocity + +:math:`p_g = ` fluid pressure + +:math:`tau = ` viscous stress tensor + +:math:`g = ` gravitational acceleration + +:math:`\beta_p = ` drag coefficient associated with a particle + +:math:`V_p = ` velocity associated with a particle + Below are the governing equations for the fluid: Conservation of fluid mass: @@ -9,12 +27,12 @@ Conservation of fluid mass: Conservation of fluid momentum: -.. math:: \frac{ \partial (\varepsilon_g \rho_g U)}{\partial t} + \nabla \cdot (\varepsilon_g \rho_g U_g U_g) + \varepsilon_g \nabla p_g = \nabla \cdot \tau + {\bf g} - + \sum_{part} \beta (V_{part} - U_g) +.. math:: \frac{ \partial (\varepsilon_g \rho_g U)}{\partial t} + \nabla \cdot (\varepsilon_g \rho_g U_g U_g) + \varepsilon_g \nabla p_g = \nabla \cdot \tau + + \sum_{part} \beta_p (V_p - U_g) + \rho_g g -Conservation of fluid volume: +where :math:`\sum_p \beta_p (V_p - U_g)` is the drag term in which :math:`V_p` represents the particle velocity. -where :math:`\sum_{part} \beta (V_{part} - U_g)` is the drag term in which :math:`V_{part}` represents the particle velocity. +Conservation of fluid volume: .. math:: \frac{\partial \varepsilon_g}{\partial t} + \nabla \cdot (\varepsilon_g U_g) = 0 -- GitLab