Heat Transfer by Conduction through a Plane Wall

on . Posted in Thermodynamics

      

heat conduction plain wall 2

Heat Transfer by Conduction Through a Plane Wall Formula

\( Q_c \;=\;  \dfrac{ - k \cdot A_c \cdot ( T_2  - T_1 )  }{  l }\) 
Symbol English Metric
\(Q_c \) = heat transfer by conduction \(Btu\;/\;hr\) \(W\)
\(A_c \) = area cross-section \(in^2\) \(mm^2\)
\( T_1 \) = temperature of one surface of the wall \(F\) \(K\)
\( T_2 \) = temperature of the other surface of the wall \(F\) \(K\)
\( k \) = thermal conductivity \(Btu-ft\;/\;hr-ft^2-F\) \(W\;/\;m-K\)
\( l \) = thickness of material \(in\) \(mm\)

 

Heat Transfer by Conduction Through a Cylindrical Wall Formula

\( Q_c \;=\;  \dfrac{ 2 \cdot \pi \cdot k \cdot l \cdot ( T_1 - T_2 )  }{ ln \cdot \left( \dfrac{ r_2 }{ r_1 } \right)  }\) 
Symbol English Metric
\( Q_c \) = heat transfer by conduction \(Btu\;/\;hr\) \(W\)
\( A_c \) = area cross-section \(in^2\) \(mm^2\)
\( \pi \) = Pi \(3.141 592 653 ...\) \(3.141 592 653 ...\)
\( r_1 \) = radius of one surface of the wall \(in\) \(mm\)
\( r_2 \) = radius of the other surface of the wall \(in\) \(mm\)
\( T_1 \) = temperature of one surface of the wall \(F\) \(K\)
\( T_2 \) = temperature of the other surface of the wall \(F\) \(K\)
\( k \) = thermal conductivity \(Btu-ft\;/\;hr-ft^2-F\) \(W\;/\;m-K\)
\( l \) = thickness of material \(in\) \(mm\)

 

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Tags: Heat Transfer Heat