From c7c0f1c973f92d2d23c5b243f3a8ce961a1b3898 Mon Sep 17 00:00:00 2001
From: Ann Almgren <asalmgren@lbl.gov>
Date: Thu, 18 Oct 2018 16:36:25 -0700
Subject: [PATCH] Update for consistency

---
 docs/source/FluidEquations.rst | 2 +-
 1 file changed, 1 insertion(+), 1 deletion(-)

diff --git a/docs/source/FluidEquations.rst b/docs/source/FluidEquations.rst
index 92684f1..125b3ff 100644
--- a/docs/source/FluidEquations.rst
+++ b/docs/source/FluidEquations.rst
@@ -25,7 +25,7 @@ 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
-           + \sum_{part} \beta_p (V_p - U_g) + \rho_g g
+           + \sum_p \beta_p (V_p - U_g) + \rho_g g
 
 where :math:`\sum_p \beta_p (V_p - U_g)` is the drag term in which :math:`V_p` represents the particle velocity and :math:`\beta_p` is the drag coefficient associated with that particle
 
-- 
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