Grammar corrections and fixing documentation error

doc/content/bib/documentation.bib

@@ -53,6 +53,7 @@ @article{greenberg1993electron
   pages={8126--8133},
   year={1993},
   publisher={American Institute of Physics}
+}
   
 
 @article{hagelaar2000boundary,

doc/content/source/bcs/ElectronAdvectionDoNothingBC.md

@@ -5,7 +5,7 @@
 ## Overview
 
 `ElectronAdvectionDoNothingBC` is an outflow boundary condition where the outflow at the
-boundary is equal to the bulk election advection equation.
+boundary is equal to the bulk electron advection equation.
 `ElectronAdvectionDoNothingBC` assumes the electrostatic approximation for the electric field.
 
 The outflow is defined as

doc/content/source/bcs/NeumannCircuitVoltageMoles_KV.md

@@ -16,10 +16,15 @@ Where $V_\text{source}$ is the driven potential, $V_\text{cathode}$ is the poten
 $e$ is the elemental charge , $\Gamma_i$ and $\Gamma_e$ are the ion and and electron particle fluxes, respectively, $A$ is the cross-sectional area of the plasma, and $R$ is the ballast resistance. Within `NeumannCircuitVoltageMoles_KV`, the charged species' flux at the boundary is assumed to be given by:
 
 \begin{equation}
-a =
+a_{e} =
 \begin{cases}
 1, & \mu_{e} \left( \nabla (V) \right) \cdot \textbf{n} > 0\\
-0, & \mu_{i} \left( \text{-} \nabla (V) \right)\cdot \textbf{n} \leq 0\\
+0, & \mu_{e} \left( \nabla (V) \right)\cdot \textbf{n} \leq 0\\
+\end{cases} \\[10pt]
+a_{i} =
+\begin{cases}
+1, & \mu_{i} \left( - \nabla (V) \right) \cdot \textbf{n} > 0\\
+0, & \mu_{i} \left( - \nabla (V) \right)\cdot \textbf{n} \leq 0\\
 \end{cases} \\[10pt]
 \Gamma_{e} \cdot \textbf{n} = \frac{1-r_{e}}{1+r_{e}} \left[ -(2 a_{e}-1) \ \mu_{e} 
 \left(\text{-} \nabla (V) \right)

doc/content/source/bcs/SecondaryElectronBC.md

@@ -8,10 +8,15 @@
 `SecondaryElectronBC` assumes the electrostatic approximation for the electric field.
 
 \begin{equation}
-a =
+a_{e} =
 \begin{cases}
-1, & \mu_{e} \left( \nabla (V) \right)  \cdot \textbf{n} > 0\\
-0, & \mu_{j} \left( \text{-} \nabla (V) \right) \cdot \textbf{n} \leq 0\\
+1, & \mu_{e} \left( \nabla (V) \right) \cdot \textbf{n} > 0\\
+0, & \mu_{e} \left( \nabla (V) \right)\cdot \textbf{n} \leq 0\\
+\end{cases} \\[10pt]
+a_{i} =
+\begin{cases}
+1, & \mu_{i} \left( - \nabla (V) \right) \cdot \textbf{n} > 0\\
+0, & \mu_{i} \left( - \nabla (V) \right)\cdot \textbf{n} \leq 0\\
 \end{cases} \\[10pt]
 \Gamma_{e} \cdot \textbf{n} = \frac{1 - r_{e}}{1 + r_{e}} \frac{\text{-}1}{2} v_{\text{th},e} n_{\gamma} - \frac{2}{1+r} (1 - a_{e}) \gamma \Gamma_{j} \cdot \textbf{n} \\[10pt]
 \Gamma_{j} \cdot \textbf{n} = \frac{1-r_{j}}{1+r_{j}} \left[ (2 a_{j}-1) \ \mu_{j}

doc/content/source/bcs/SecondaryElectronEnergyBC.md

@@ -8,10 +8,15 @@
 `SecondaryElectronEnergyBC` assumes the electrostatic approximation for the electric field.
 
 \begin{equation}
-a =
+a_{e} =
 \begin{cases}
 1, & \mu_{e} \left( \nabla (V) \right) \cdot \textbf{n} > 0\\
-0, & \mu_{j} \left( \text{-} \nabla (V) \right) \cdot \textbf{n} \leq 0\\
+0, & \mu_{e} \left( \nabla (V) \right)\cdot \textbf{n} \leq 0\\
+\end{cases} \\[10pt]
+a_{i} =
+\begin{cases}
+1, & \mu_{i} \left( - \nabla (V) \right) \cdot \textbf{n} > 0\\
+0, & \mu_{i} \left( - \nabla (V) \right)\cdot \textbf{n} \leq 0\\
 \end{cases} \\[10pt]
 \Gamma_{\epsilon} \cdot \textbf{n} = \frac{1 - r_{e}}{1 + r_{e}} \frac{\text{-}5}{6} v_{\text{th},e} n_{\gamma} \varepsilon_{\gamma} - \frac{5}{3} \frac{2}{1+r} (1 - a_{e}) \gamma \Gamma_{j} \cdot \textbf{n} \\[10pt]
 \Gamma_{j} \cdot \textbf{n} = \frac{1-r_{j}}{1+r_{j}} \left[ (2 a_{j}-1) \ \mu_{j}

doc/tutorial_pdf/Zapdos_Tutorial.tex

@@ -541,7 +541,7 @@
 
   \begin{verbatim}
   [InterfaceKernels]
-    #Defining election advection to the water
+    #Defining electron advection to the water
     [em_advection]
         type = InterfaceAdvection
         mean_en_neighbor = mean_en
@@ -552,7 +552,7 @@
         position_units = ${dom1Scale}
         neighbor_position_units = ${dom0Scale}
     []
-    #Defining election diffusion to the water
+    #Defining electron diffusion to the water
     [em_diffusion]
         type = InterfaceLogDiffusionElectrons
         mean_en_neighbor = mean_en

src/bcs/ElectronAdvectionDoNothingBC.C

@@ -19,8 +19,8 @@ ElectronAdvectionDoNothingBC::validParams()
   params.addRequiredCoupledVar(
       "potential", "The gradient of the potential will be used to compute the advection velocity.");
   params.addRequiredParam<Real>("position_units", "The units of position.");
-  params.addClassDescription("Boundary condition where the election advection flux at the boundary "
-                             "is equal to the bulk election advection equation");
+  params.addClassDescription("Boundary condition where the electron advection flux at the boundary "
+                             "is equal to the bulk electron advection equation");
   return params;
 }
 

src/bcs/ElectronDiffusionDoNothingBC.C

@@ -17,8 +17,8 @@ ElectronDiffusionDoNothingBC::validParams()
 {
   InputParameters params = ADIntegratedBC::validParams();
   params.addRequiredParam<Real>("position_units", "Units of position");
-  params.addClassDescription("Boundary condition where the election diffusion flux at the boundary "
-                             "is equal to the bulk election diffusion equation");
+  params.addClassDescription("Boundary condition where the electron diffusion flux at the boundary "
+                             "is equal to the bulk electron diffusion equation");
   return params;
 }