Changes

Steady-State Thermal Analysis

193 bytes added, 19:10, 16 June 2018
<math> T(\mathbf{r}) = T_0 </math>
The Neuman boundary condition constrains the heat flow through the domain boundary walls:
 
<math>q = -k \frac{\partial T}{\partial n} = -k \mathbf{\hat{n}) . \nabla T(\mathbf{r}) = q_s </math>
Kazem Sabet
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