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The Society of Fire Protection Engineers (SFPE) has developed a standard entitled {\em S.02 -- Calculation Methods to Predict the Thermal Performance of Structures \& Fire Resistive Assemblies}~\cite{SFPE_S.02} that contains an appendix with verification cases to benchmark basic heat transfer calculations. This section contains several of these cases.
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\subsection{Case 1: Lumped Mass Subjected to Standard Fire}
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\label{SFPE_Case_1}
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A plate ($\rho=7850$~kg/m$^3$, $c=0.52$~kJ/(kg~K), $\epsilon=0.7$) that has a thickness of 4~cm and an initial temperature of 20~°C is heated on the top and bottom surfaces according to the standard ISO~834 fire curve
where the time, $t$, is in seconds. If the thermal conductivity of the material is relatively large, the temperature in the section can be taken as uniform. For the convection heat transfer coefficient, $h=25$~W/(m$^2$~K), calculate the temperature of the plate as a function of time (Fig.~\ref{fig:SFPE_Case_1}).
\caption[The SFPE heat transfer verification Case 1]{Temperature of a 4~cm thick plate that is heated top and bottom by the standard fire curve.}
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\label{fig:SFPE_Case_1}
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\end{figure}
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\FloatBarrier
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\subsection{Case 2: Lumped Mass Subjected to Incident Flux}
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\label{SFPE_Case_2}
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A 1~cm thick horizontal flat plate ($\rho=7850$~kg/m$^3$, $c=0.56$~kJ/(kg~K), $\epsilon=0.9$) with an initial temperature of 20~°C is exposed from above with a radiant heater set to an incident flux of ̇50~kW/m$^2$. The gas temperature is 20~°C and $h=12$~W/(m$^2$~K). Assuming that the bottom and sides of the plate are perfectly insulated, and that the thermal conductivity of the material is sufficiently large to assume a uniform temperature with depth, calculate the temperature of the plate as a function of time (Fig.~\ref{fig:SFPE_Case_2}).
\caption[The SFPE heat transfer verification Case 2]{Temperature of a 1~cm thick plate that is heated on top via an incident flux and insulated below.}
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\label{fig:SFPE_Case_2}
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\end{figure}
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\FloatBarrier
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\subsection{Case 6: 2-D Heat Transfer with Cooling by Convection}
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\label{SFPE_Case_6}
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@@ -5039,11 +5072,7 @@ \subsection{Case 6: 2-D Heat Transfer with Cooling by Convection}
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\subsection{Case 7: 2-D Heat Transfer by Convection and Radiation}
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\label{SFPE_Case_7}
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A 0.2 m by 0.2 m square column ($k=1$~W/(m~K), $\rho=2400$~kg/m$^3$, $c=1$~kJ/(kg~K), $\epsilon=0.8$) is heated according to the ISO~834 time-temperature curve
where the time, $t$, is in seconds. Assuming that $h=10$~W/(m$^2$~K) and that the initial temperature is $T_\infty=273$~K, calculate the temperature at the column center, corner and middle side surface as a function of time (Fig.~\ref{fig:SFPE_Case_7}).
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A 0.2 m by 0.2 m square column ($k=1$~W/(m~K), $\rho=2400$~kg/m$^3$, $c=1$~kJ/(kg~K), $\epsilon=0.8$) is heated according to the ISO~834 time-temperature curve, Eq.~(\ref{ISO_834}). Assuming that $h=10$~W/(m$^2$~K) and that the initial temperature is $T_\infty=273$~K, calculate the temperature at the column center, corner and middle side surface as a function of time (Fig.~\ref{fig:SFPE_Case_7}).
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