LW Engr Ref doc errors

doc/engineering-reference/src/simulation-models-encyclopedic-reference-003/indoor-living-wall.tex

@@ -33,12 +33,12 @@ \subsection{Energy Balance of Indoor Living Wall}\label{energy-balance-of-indoor
 Indoor air heat balance connects with indoor living walls through convective heat transfer, which has the opposite sign of the term in surface heat balance. Convective portion of heat gain from LED lights also contributes to zone air heat balance equation.
 
 \begin{equation}
-\begin{array}{l}{\rho_{air}}{V_z}{c_p}{dT_z}/{dt} = \sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^{}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} ({{T_{si}} - {T_z}}) + {{h_ip}}{A_ip}({{T_{p}} - {T_z}})\\ + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{{T_{zi}} - {T_z}} + {\dot m_{\inf }}{C_p}( {{T_\infty } - {T_z}}) +{\dot Q_{sys}}\right)\end{array}
+\begin{array}{l}{\rho_{air}}{V_z}{c_p}{dT_z}/{dt} = \sum\limits_{i = 1}^{{N_{sl}}} {\dot Q_i^{}}  + \sum\limits_{i = 1}^{{N_{surfaces}}} {{h_i}} {A_i} ({{T_{si}} - {T_z}}) + {{h_ip}}{A_ip}({{T_{p}} - {T_z}})\\ + \sum\limits_{i = 1}^{{N_{zones}}} {{{\dot m}_i}} {C_p}{{T_{zi}} - {T_z}} + {\dot m_{\inf }}{C_p}( {{T_\infty } - {T_z}}) +{\dot Q_{sys}})\end{array}
 \end{equation} 
 
 where:
 
-\({\rho_{air}}{V_z}{c_p}\(dT_z}/{dt}\) represents energy stored in zone air during each timestep (W);  
+\({\rho_{air}}{V_z}{c_p}{dT_z}/{dt}\) represents energy stored in zone air during each timestep (W);  
 
 \({\rho_{air}}\) is zone air density (kg/m\(^3\));
 
@@ -71,7 +71,7 @@ \subsection{Energy Balance of Indoor Living Wall}\label{energy-balance-of-indoor
 
 \(W\) is the humidity ratio of moisture air (kg moisture/kg dry air);  
 
-\({\rho_{air}}{V_z}{C_W}{({\delta t})^{ - 1}})({W_z^t - W_z^{t - \delta t}}) \right)\) represents moisture stored in zone air during each timestep (kg/s);
+\({\rho_{air}}{V_z}{C_W}{({\delta t})^{ - 1}}({W_z^t - W_z^{t - \delta t}})\) represents moisture stored in zone air during each timestep (kg/s);
 
 \(kg_{mass_{et}}\) represents moisture rate from plant evapotranspiration added to zone air (kg/s);
 
@@ -115,7 +115,7 @@ \subsection{Evapotranspiration from indoor living wall}\label{evaporation-from-i
 
 \(r_a\) represents aerodynamic resistance, which is the resistance to the flow of water vapor and sensible heat from the surface of the leaf to the surrounding air (s/m).
 
-Empirical models of stomatal resistance such as the Jarvis and the Ball models require experimental data to generate submodel structure and fit the model coefficients.  In this module, we used the surface and aerodynamic resistance models from Graamans et al. to calculate r_s and r_a. 
+Empirical models of stomatal resistance such as the Jarvis and the Ball models require experimental data to generate submodel structure and fit the model coefficients.  In this module, we used the surface and aerodynamic resistance models from Graamans et al. to calculate $r_s$ and $r_a$. 
 
 \begin{equation}
 r_s=60 \cdot (1500+I_n/C)/(200+I_n/C)