Changes between Version 1 and Version 2 of doc/app/indoorequ

Timestamp:

Jul 30, 2019 8:26:25 AM (6 years ago)

Author:

srissman

Comment:

--

doc/app/indoorequ

@@ -46 +46 @@
 }}}
 
-To take respect of an non rectangular building a virtual façade area specific indoor volume shown in figure 1, created.
-
-FIGURE 1
+To take respect of an non rectangular building a virtual façade area specific indoor volume shown in figure 1, created.\\
+
+ [[Image(virtual_volume.png,300px, border=0)]]
 
 {{{
@@ -89 +89 @@
 The ICM is based on an analytical solution of Fourier’s law considering a resistance model with five resistances ''R'' [K/W] and one heat capacity ''C'' [J/K] as seen in figure 2. 
 
-FIGURE 2
+[[Image(5R1C_scheme.png,400px, border=0)]]
 
 The solution is based on a Crank-Nicolson scheme for a one-hour time step. Since the calculations are based on heat transfer coefficients, ''H'' [W/K] all figures and equations are based on heat transfer coefficients. This is the reciprocal value of ''R'' and takes short wave, long wave, convective and conductive heat transfer and heat transport (by air) into account.
@@ -155 +155 @@
 #!Latex
 \begin{align*}
-  & H_{t,1} = \frac{1}{ \frac{1}{H_{v}} \ + \frac{1}{H_{t,is}} \ } \
-\end{align*}
-}}}
-{{{
-#!Latex
-\begin{align*}
-  & H_{t,2} = H_{t,1} + H_{t,es}
-\end{align*}
-}}}
-{{{
-#!Latex
-\begin{align*}
+  & H_{t,1} = \frac{1}{ \frac{1}{H_{v}} \ + \frac{1}{H_{t,is}} \ } \ \\
+  & H_{t,2} = H_{t,1} + H_{t,es} \\
   & H_{t,3} = \frac{1}{ \frac{1}{H_{t,2}} \ + \frac{1}{H_{t,ms}} \ } \
 \end{align*}
@@ -258 +248 @@
 \end{align*}
 }}}
+
 '''Heating and Cooling Demand'''\\
+
 The heating and cooling demand ''Φ'',,HC,nd,, is disposed in 5 different stages as shown in figure 3. \\
-FIGURE 3\\
+
+[[Image(Phi_HCnd_scheme.png,400px, border=0)]]
+
 Stage 1: No heating or cooling necessary, because room temperature ''ϑ'',,air,, is between the set comfort temperatures when heating ''ϑ'',,heat,set,, or cooling ''ϑ'',,cool,set,, is needed.
 In this case the demand is: