diff --git a/src/equations/compressible_euler_2d.jl b/src/equations/compressible_euler_2d.jl
index fa2c9f5e94f..3c6f759db2b 100644
--- a/src/equations/compressible_euler_2d.jl
+++ b/src/equations/compressible_euler_2d.jl
@@ -847,7 +847,7 @@ end
     p = 0.5 * (p_ll + p_rr) - 0.5 * c * rho * (v_rr - v_ll)
     v = 0.5 * (v_ll + v_rr) - 1 / (2 * c * rho) * (p_rr - p_ll)
 
-    # We treat the energy term in analogy to the potential temperature term in the paper by
+    # We treat the energy term analogous to the potential temperature term in the paper by
     # Chen et al., i.e. we use p_ll and p_rr, and not p
     if v >= 0
         f1, f2, f3, f4 = v * u_ll
@@ -885,7 +885,7 @@ end
     p = 0.5 * (p_ll + p_rr) - 0.5 * c * rho * (v_rr - v_ll) / norm_
     v = 0.5 * (v_ll + v_rr) - 1 / (2 * c * rho) * (p_rr - p_ll) * norm_
 
-    # We treat the energy term in analogy to the potential temperature term in the paper by
+    # We treat the energy term analogous to the potential temperature term in the paper by
     # Chen et al., i.e. we use p_ll and p_rr, and not p
     if v >= 0
         f1, f2, f3, f4 = u_ll * v
diff --git a/src/equations/compressible_euler_3d.jl b/src/equations/compressible_euler_3d.jl
index db74f1f5485..292b912f009 100644
--- a/src/equations/compressible_euler_3d.jl
+++ b/src/equations/compressible_euler_3d.jl
@@ -967,7 +967,7 @@ References:
     p = 0.5 * (p_ll + p_rr) - 0.5 * c * rho * (v_rr - v_ll)
     v = 0.5 * (v_ll + v_rr) - 1 / (2 * c * rho) * (p_rr - p_ll)
 
-    # We treat the energy term in analogy to the potential temperature term in the paper by
+    # We treat the energy term analogous to the potential temperature term in the paper by
     # Chen et al., i.e. we use p_ll and p_rr, and not p
     if v >= 0
         f1, f2, f3, f4, f5 = v * u_ll
@@ -1009,7 +1009,7 @@ end
     p = 0.5 * (p_ll + p_rr) - 0.5 * c * rho * (v_rr - v_ll) / norm_
     v = 0.5 * (v_ll + v_rr) - 1 / (2 * c * rho) * (p_rr - p_ll) * norm_
 
-    # We treat the energy term in analogy to the potential temperature term in the paper by
+    # We treat the energy term analogous to the potential temperature term in the paper by
     # Chen et al., i.e. we use p_ll and p_rr, and not p
     if v >= 0
         f1, f2, f3, f4, f5 = v * u_ll