diff --git a/.github/workflows/ex-rtd.yml b/.github/workflows/ex-rtd.yml
index 8096c451..20e90e50 100644
--- a/.github/workflows/ex-rtd.yml
+++ b/.github/workflows/ex-rtd.yml
@@ -115,7 +115,7 @@ jobs:
           pandoc --version
 
       - name: Setup pixi
-        uses: prefix-dev/setup-pixi@v0.9.3
+        uses: prefix-dev/setup-pixi@v0.9.4
         with:
           pixi-version: v0.41.4
           manifest-path: modflow6-examples/pixi.toml
diff --git a/.github/workflows/ex-workflow.yml b/.github/workflows/ex-workflow.yml
index 4c13f256..6e53a61a 100644
--- a/.github/workflows/ex-workflow.yml
+++ b/.github/workflows/ex-workflow.yml
@@ -30,7 +30,7 @@ jobs:
         uses: actions/checkout@v6
 
       - name: Setup pixi
-        uses: prefix-dev/setup-pixi@v0.9.3
+        uses: prefix-dev/setup-pixi@v0.9.4
         with:
           pixi-version: v0.41.4
 
@@ -60,7 +60,7 @@ jobs:
           path: modflow6
 
       - name: Setup pixi
-        uses: prefix-dev/setup-pixi@v0.9.3
+        uses: prefix-dev/setup-pixi@v0.9.4
         with:
           pixi-version: v0.41.4
           manifest-path: modflow6-examples/pixi.toml
@@ -133,7 +133,7 @@ jobs:
           path: usgslatex
 
       - name: Setup pixi
-        uses: prefix-dev/setup-pixi@v0.9.3
+        uses: prefix-dev/setup-pixi@v0.9.4
         with:
           pixi-version: v0.41.4
           manifest-path: modflow6-examples/pixi.toml
diff --git a/doc/sections/ex-gwt-adv-schemes.tex b/doc/sections/ex-gwt-adv-schemes.tex
index 2421b2da..db49d571 100644
--- a/doc/sections/ex-gwt-adv-schemes.tex
+++ b/doc/sections/ex-gwt-adv-schemes.tex
@@ -22,7 +22,7 @@ \subsection{Example description}
 \item \textbf{Voronoi grid}: Grid using Voronoi cells derived from triangular cells
 \end{itemize}
 
-\noindent The simulation time spans 300 seconds using adaptive time stepping with an initial time step of 5 seconds and a Courant number of 0.7. The Courant number is a dimensionless quantity representing the fraction of a cell that fluid travels in a single time step. A value less or equal to 1 is required for stability of the central-difference scheme. A relatively high Courant number is chosen here specifically to challenge the central difference scheme and demonstrate its potential for oscillatory behavior on discontinuous functions. Four advection schemes are compared:
+\noindent The simulation time spans 300 seconds using adaptive time stepping with an initial time step of 5 seconds and a Courant number of 0.7. The Courant number is a dimensionless quantity representing the fraction of a cell that fluid travels in a single time step. A value less or equal to 1 is required for stability. A relatively high Courant number is chosen here specifically to challenge the central difference scheme and demonstrate its potential for oscillatory behavior on discontinuous functions. Four advection schemes are compared:
 \begin{itemize}
 \item \textbf{Upstream}: First-order accurate, stable but diffusive scheme
 \item \textbf{Central difference}: Second-order accurate but prone to oscillations on discontinuities
@@ -102,7 +102,7 @@ \subsubsection{Key Findings}
 \begin{enumerate}
 \item \textbf{Grid-dependent performance}: The central difference scheme performed reasonably on the structured grid but became unstable on the triangular and Voronoi grids, particularly for the discontinuous input concentration profiles. This demonstrates the critical importance of considering grid type when selecting numerical schemes.
 
-\item \textbf{Courant number sensitivity}: The central difference scheme's stability was highly sensitive to the Courant number. At Courant = 0.7, it exhibited undershoots leading to negative concentrations on smooth functions and oscillartory instability for the discontinuous inflow concentration profiles. Reducing the Courant number by reducing the time step size mitigated these issues for the smooth inflow concentration profile but at the cost of computational efficiency.
+\item \textbf{Courant number sensitivity}: The central difference scheme's stability was highly sensitive to the Courant number. At Courant = 0.7, it exhibited undershoots leading to negative concentrations on smooth functions and oscillartory instability for the discontinuous inflow concentration profiles. Reducing the Courant number mitigated these issues for the smooth inflow concentration profile but at the cost of computational efficiency.
 
 \item \textbf{UTVD scheme as overall best choice}: The UTVD scheme consistently outperformed all others across grid types and inflow concentration profiles. It was the least dissipative scheme that maintained stability, and is the only stable scheme that approached the maximum values of analytical solutions for sharp discontinuities.