From 23a650a85b557a46faa1be13146ad1b6ad8de799 Mon Sep 17 00:00:00 2001
From: freiler <54753719+freiler@users.noreply.github.com>
Date: Mon, 17 Jun 2024 10:59:34 -0600
Subject: [PATCH] Apply suggestions from code review #27800 #27887 #27888

Co-authored-by: Mauricio Tano <mauriciotano@gmail.com>
---
 .../doc/content/source/fvkernels/INSFVTKESourceSink.md      | 6 +++---
 1 file changed, 3 insertions(+), 3 deletions(-)

diff --git a/modules/navier_stokes/doc/content/source/fvkernels/INSFVTKESourceSink.md b/modules/navier_stokes/doc/content/source/fvkernels/INSFVTKESourceSink.md
index 44853034fdba..9cf0e29493db 100644
--- a/modules/navier_stokes/doc/content/source/fvkernels/INSFVTKESourceSink.md
+++ b/modules/navier_stokes/doc/content/source/fvkernels/INSFVTKESourceSink.md
@@ -32,7 +32,7 @@ G_k = min \left( G_k , C_{PL} \rho \epsilon \right) \,,
 
 where:
 
-- $C_{PL}$ it the limiter constant, and set to a recommended value of 10 .
+- $C_{PL}$ it the limiter constant, and set by default to a recommended value of 10 \cite{durbin1996k}.
 
 ## Wall formulation:
 
@@ -69,7 +69,7 @@ G_k = 0.0 \,,
 In the `logarithmic` boundary layers the production term is no longer negligible and is defined as:
 
 \begin{equation}
-G_k = \tau_w ||\nabla \vec{u}|| = \left( \mu_t + \mu \right) ||\nabla \vec{u}|| \frac{ C_{\mu}^{0.25} \sqrt(k)}{\kappa y_p} \,,
+G_k = \tau_w ||\nabla \vec{u}|| = \mu_w ||\nabla \vec{u}|| \frac{ C_{\mu}^{0.25} \sqrt(k)}{\kappa y_p} \,,
 \end{equation}
 
 where:
@@ -84,7 +84,7 @@ The formulation assumes that the near wall value is already imposed in the $\mu_
 When solving a linear problem, instead of the nonlinear formulation, the production term is formulated as:
 
 \begin{equation}
-G_k =  \left( \mu_t + \mu \right) ||\nabla \vec{u}|| \frac{ C_{\mu}^{0.25} k}{\sqrt{k_{old}} \kappa y_p} \,.
+G_k =  \mu_w ||\nabla \vec{u}|| \frac{ C_{\mu}^{0.25} k}{\sqrt{k_{old}} \kappa y_p} \,.
 \end{equation}
 
 where: