From 3f69afff9145a18d174a5147feda47f1c80c56a2 Mon Sep 17 00:00:00 2001
From: Katharina Heck <katharina.heck@iws.uni-stuttgart.de>
Date: Sun, 6 Oct 2019 10:05:19 +0200
Subject: [PATCH] [doc][handbook] small corrections in basics
---
doc/handbook/6_basics.tex | 4 ++--
1 file changed, 2 insertions(+), 2 deletions(-)
diff --git a/doc/handbook/6_basics.tex b/doc/handbook/6_basics.tex
index d33f2a51fc..bfcfe229cf 100644
--- a/doc/handbook/6_basics.tex
+++ b/doc/handbook/6_basics.tex
@@ -260,7 +260,7 @@ It is a value between zero and one, depending on the saturation.
The relations describing the relative permeabilities of the wetting and non-wetting phase are different
as the wetting phase predominantly occupies small pores and the edges of larger pores while the
non-wetting phases occupies large pores.
-The relative permeabilities for the wetting phase $k_\mathrm{r,w}$ and the non-wetting phase are calculated as:
+The relative permeabilities for the wetting phase $k_\mathrm{r,w}$ and the non-wetting phase are e.g. calculated as (also by \citet{brooks1964hydrau}):
\begin{equation}\label{eq:krw}
k_\mathrm{r,w} = S_\mathrm{e}^{\frac{2+3\lambda}{\lambda}}
@@ -301,7 +301,7 @@ Molecular diffusion is a process determined by the concentration gradient.
It is commonly modeled as Fickian diffusion following Fick's first law:
\begin{equation} \label{eq:Diffusion}
-\mathbf{j_d}=-\rho_{\mathrm{mol},\alpha} D^\kappa_\alpha \nabla x^\kappa_\alpha,
+\mathbf{j_d}=-\rho_{\alpha} D^\kappa_\alpha \nabla X^\kappa_\alpha,
\end{equation}
where $D^\kappa_\alpha$ is the molecular diffusion coefficient of component $\kappa$ in phase $\alpha$.
--
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