basics:building_physics_-_basics:thermal_bridges:tbcalculation:examples:unheatedb
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basics:building_physics_-_basics:thermal_bridges:tbcalculation:examples:unheatedb [2019/01/24 09:30] – cblagojevic | basics:building_physics_-_basics:thermal_bridges:tbcalculation:examples:unheatedb [2022/02/15 18:58] (current) – admin | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{\dfrac{1}{U} = \dfrac{1}{U_f} + \dfrac{A}{(A \cdot U_{bf}) + (z \cdot P \cdot U_{bw}) + (h \cdot P \cdot U_W) + (0{,}33 \cdot n \cdot V)}} | \large{\dfrac{1}{U} = \dfrac{1}{U_f} + \dfrac{A}{(A \cdot U_{bf}) + (z \cdot P \cdot U_{bw}) + (h \cdot P \cdot U_W) + (0{,}33 \cdot n \cdot V)}} | ||
- | </ | + | $$ |
\\ | \\ | ||
\\ | \\ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{\Phi = L_{iu} \cdot (\theta_i - \theta_u) + L_{ie} \cdot (\theta_i - \theta_e)} | \large{\Phi = L_{iu} \cdot (\theta_i - \theta_u) + L_{ie} \cdot (\theta_i - \theta_e)} | ||
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{\Phi = \left(\frac{L_{iu} \cdot L_{ue}}{L_{iu} + L_{ue}}\right) \cdot (\theta_i - \theta_e) \quad \Rightarrow \quad L_{2d} = \left(\frac{L_{iu} \cdot L_{ue}}{L_{iu} + L_{ue}} + L_{ie}\right)} | \large{\Phi = \left(\frac{L_{iu} \cdot L_{ue}}{L_{iu} + L_{ue}}\right) \cdot (\theta_i - \theta_e) \quad \Rightarrow \quad L_{2d} = \left(\frac{L_{iu} \cdot L_{ue}}{L_{iu} + L_{ue}} + L_{ie}\right)} | ||
- | </ | + | $$ |
</ | </ | ||
Thus $L_{ie}$ , $L_{iu}$ and $L_{ue}$ | Thus $L_{ie}$ , $L_{iu}$ and $L_{ue}$ | ||
- | <WRAP centeralign> | + | <WRAP centeralign> |
- | <latex> | + | $$ |
- | $$ \bordermatrix{ | + | \begin{matrix} |
- | & L_{iu} & L_{ie} & L_{ue} \cr | + | & \begin{matrix}L_{iu}& |
- | L_1 & 1 & 1 & 0 \cr | + | \begin{matrix}L_1\\\\L_2\\\\L_3\end{matrix} |
- | L_2 & 0 & 1 & 1 \cr | + | & \begin{pmatrix}1\quad&1\quad&0\quad\\\\0\quad&1\quad&1\quad\\\\1\quad&0\quad&1\quad\end{pmatrix}\\\\ |
- | L_3 & 1 & 0 & 1 \cr | + | \end{matrix} |
- | } | + | |
\quad \Rightarrow \quad | \quad \Rightarrow \quad | ||
\begin{matrix} | \begin{matrix} | ||
- | L_{iu} = 0{.}5 \cdot (L_1-L_2+L_3) \\ | + | L_{iu} = 0{,}5 \cdot (L_1-L_2+L_3) \\ |
- | L_{is} = 0{.}5 \cdot (L_1+L_2-L_3) \\ | + | L_{ie} = 0{,}5 \cdot (L_1+L_2-L_3) \\ |
- | L_{us} = 0{.}5 \cdot (L_2+L_3-L_1) | + | L_{ue} = 0{,}5 \cdot (-L_1+L_2+L_3) |
\end{matrix} | \end{matrix} | ||
$$ | $$ | ||
- | </ | ||
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
**Determining the conductance** | **Determining the conductance** | ||
- | < | + | $$ |
\Large{_{2d}} | \Large{_{2d}} | ||
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{ | \large{ | ||
- | $$L_{iu} = 0{.}5 \cdot (L_1-L_2+L_3) = 0{.}5540 \, \frac{\text{W}}{\text{m} \cdot \text{K}}} $$\\ | + | L_{iu} = 0{.}5 \cdot (L_1-L_2+L_3) = 0{.}5540 \, \frac{\text{W}}{\text{m} \cdot \text{K}} \\ |
- | $$L_{is} = 0{.}5 \cdot (L_1+L_2-L_3) = 0{.}2314 \, \frac{\text{W}}{\text{m} \cdot \text{K}}} $$\\ | + | L_{is} = 0{.}5 \cdot (L_1+L_2-L_3) = 0{.}2314 \, \frac{\text{W}}{\text{m} \cdot \text{K}} \\ |
- | $$L_{us} = 0{.}5 \cdot (-L_1+L_2+L_3) = 2{.}6177 \, \frac{\text{W}}{\text{m} \cdot \text{K}}}$$} | + | L_{us} = 0{.}5 \cdot (-L_1+L_2+L_3) = 2{.}6177 \, \frac{\text{W}}{\text{m} \cdot \text{K}}} |
- | </ | + | $$ |
</ | </ | ||
<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
- | \large{L_{2d} = \left(\frac{L_{iu} \cdot L_{ue}}{L_{iu} + L_{ue}} + L_{ie}\right) = 0{.}6886 \, \frac{\text{W}}{\text{m} \cdot \text{K}}}} | + | \large{L_{2d} = \left(\frac{L_{iu} \cdot L_{ue}}{L_{iu} + L_{ue}} + L_{ie}\right) = 0{.}6886 \, \frac{\text{W}}{\text{m} \cdot \text{K}}} |
- | </ | + | $$ |
</ | </ | ||
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Therefore: | Therefore: | ||
<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
- | $$\dfrac{1}{U} = \dfrac{1}{U_f} + \dfrac{A}{(A \cdot U_{bf}) + (z \cdot P \cdot U_{bw}) + (h \cdot P \cdot U_W) + (0{.}33 \cdot n \cdot V)} | + | \dfrac{1}{U} = \dfrac{1}{U_f} + \dfrac{A}{(A \cdot U_{bf}) + (z \cdot P \cdot U_{bw}) + (h \cdot P \cdot U_W) + (0{.}33 \cdot n \cdot V)} |
\quad \Rightarrow \quad | \quad \Rightarrow \quad | ||
- | U = 0{.}1273 \, \dfrac{\text{W}}{\text{m}^2 \cdot \text{K}}}$$ | + | U = 0{.}1273 \, \dfrac{\text{W}}{\text{m}^2 \cdot \text{K}} |
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | ||
$$\Psi_g = L_{2d}-l_{AW} \cdot U_{AW}-0{.}5 \cdot B' \cdot U$$ | $$\Psi_g = L_{2d}-l_{AW} \cdot U_{AW}-0{.}5 \cdot B' \cdot U$$ | ||
- | </ | ||
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$\Psi_g = 0{.}689 \, \dfrac{\text{W}}{\text{m} \cdot \text{K}} \, - \, 1{.}830 \, \text{m} \, \cdot \, 0{.}120 \, \dfrac{\text{W}}{\text{m}^2 \cdot \text{K}} \, - \, 0{.}5 \, \cdot \, 8 \, \text{m} \, \cdot \, 0{.}1273 \, \dfrac{\text{W}}{\text{m}^2 \cdot \text{K}} = -0{.}042 \, \dfrac{\text{W}}{\text{m} \cdot \text{K}}$$ |
- | $$\Psi_g = 0{.}687 \, \dfrac{\text{W}}{\text{m} \cdot \text{K}}} \, - \, 1{.}830 \, \text{m} \, \cdot \, 0{.}120 \, \dfrac{\text{W}}{\text{m}^2 \cdot \text{K}}} \, - \, 0{.}5 \, \cdot \, 8 \, \text{m} \, \cdot \, 0{.}1273 \, \dfrac{\text{W}}{\text{m}^2 \cdot \text{K}}} = -0{.}042 \, \dfrac{\text{W}}{\text{m} \cdot \text{K}}}$$ | + | |
- | </ | + | |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
**Determining the conductance** | **Determining the conductance** | ||
- | < | + | $ |
\Large{L_{2d}} | \Large{L_{2d}} | ||
- | </ | + | $ |
</ | </ | ||
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**Ψ-value (proportion of exterior wall)** | **Ψ-value (proportion of exterior wall)** | ||
</ | </ | ||
+ | |||
<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
- | \large{\Psi_g = L_{ie}-l_{AW} \cdot U_{AW}$} | + | \large{\Psi_g = L_{ie}-l_{AW} \cdot U_{AW}} |
- | </ | + | $$ |
</ | </ | ||
<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{\Psi_{exterior wall} = 0{.}231-1{.}830 \cdot 0{.}120 = 0{.}0114} | \large{\Psi_{exterior wall} = 0{.}231-1{.}830 \cdot 0{.}120 = 0{.}0114} | ||
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{\Psi_g = L_{iu}-0{.}5 \cdot B' \cdot U_{basement ceiling}} | \large{\Psi_g = L_{iu}-0{.}5 \cdot B' \cdot U_{basement ceiling}} | ||
- | </ | + | $$ |
</ | </ | ||
<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{\Psi_{basement ceiling} = 0{.}5543-0{.}5 \cdot 8 \cdot 0{.}148 = -0{.}0377} | \large{\Psi_{basement ceiling} = 0{.}5543-0{.}5 \cdot 8 \cdot 0{.}148 = -0{.}0377} | ||
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{U_{f, | \large{U_{f, | ||
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{\theta_{basement} = \theta_i-f_x \cdot (\theta_i - \theta_e) = 20 \, ^\circ C - 0{.}6 \cdot (20 \, ^\circ C - (-10 \, ^\circ C)) = 2 \, ^\circ C} | \large{\theta_{basement} = \theta_i-f_x \cdot (\theta_i - \theta_e) = 20 \, ^\circ C - 0{.}6 \cdot (20 \, ^\circ C - (-10 \, ^\circ C)) = 2 \, ^\circ C} | ||
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
**Determining the minimum surface temperature and** | **Determining the minimum surface temperature and** | ||
- | < | + | $$ |
\Large{f_{Rsi}} | \Large{f_{Rsi}} | ||
- | </ | + | $$ |
</ | </ | ||
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<WRAP centeralign> | <WRAP centeralign> | ||
- | < | + | $$ |
\large{f_{Rsi} = \dfrac{17{.}6 - (-10)}{20-(-10)}=0{.}92} | \large{f_{Rsi} = \dfrac{17{.}6 - (-10)}{20-(-10)}=0{.}92} | ||
- | </ | + | $$ |
</ | </ | ||
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===== See also ===== | ===== See also ===== | ||
- | * [[basics: | + | * [[basics: |
- | * [[basics: | + | * [[basics: |
- | * [[basics: | + | * [[basics: |
+ | |||
basics/building_physics_-_basics/thermal_bridges/tbcalculation/examples/unheatedb.1548318654.txt.gz · Last modified: 2019/01/24 09:30 by cblagojevic