diff --git a/doc/cases.tex b/doc/cases.tex
index db1dfb50..20a5c271 100644
--- a/doc/cases.tex
+++ b/doc/cases.tex
@@ -284,7 +284,7 @@ \subsubsection{Turbulence under breaking surface waves}\label{breaking_waves}
 \sect{sec:updategrid}.  If you want to compare the computed profiles
 with the analytical solutions in \eq{power_law}, you'll need a
 specification of the parameter $K$. This parameter is computed in {\tt
-k\_bc()} to be found in {\tt turbulence.F90}, where you can add a few
+k\_bc()} to be found in {\tt turbulence.F90}, where you can add a few
 FORTRAN lines to write it out.
 
 \subsubsection{Some entrainment scenarios}\label{entrainment}
diff --git a/doc/turbulenceIntro.tex b/doc/turbulenceIntro.tex
index c097fe18..b3b72802 100644
--- a/doc/turbulenceIntro.tex
+++ b/doc/turbulenceIntro.tex
@@ -1027,7 +1027,7 @@ \subsection{Numerics}
 l$-equation and the $\epsilon$-equation (described in
 \sect{sec:lengthscaleeq} and \sect{sec:dissipationeq}), 
 $Q$ would be proportional to $q/l$ and $\epsilon
-/kĻ$, repsectively.
+/k$, respectively.
 
 A straight-forward, explicit discretisation in time of \eq{eq:burchard11}
 can be written as