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1. Context
The design of the convection article is very different from that of the conduction article. In the latter case, the entire temperature field must be determined as a function of place and time throughout the solid. This is done in three steps. The general solution of the heat equation is obtained in a first step by analytical or, in most cases, numerical resolutions. In a second step, some of the integration constants are determined by considering the thermal boundary conditions. This is sufficient for stationary conduction
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