2-21 We consider a thin element of thickness Ar in a large plane wall (see Fig. 2-13 in the text). The density of the wall is p, the specific heat is C, and the area of the wall normal to the direction of heat transfer is A. In the absence of any heat generation, an energy balance on this thin element of thickness Ar during a small time interval At can be expressed as

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Chapter 2 Heat Conduction Equation
2-21 We consider a thin element of thickness Ar in a large plane wall (see Fig. 2-13 in the text). The
density of the wall is p, the specific heat is C, and the area of the wall normal to the direction of heat
transfer is A. In the absence of any heat generation, an energy balance on this thin element of thickness Ar
during a small time interval At can be expressed as
Transcribed Image Text:Chapter 2 Heat Conduction Equation 2-21 We consider a thin element of thickness Ar in a large plane wall (see Fig. 2-13 in the text). The density of the wall is p, the specific heat is C, and the area of the wall normal to the direction of heat transfer is A. In the absence of any heat generation, an energy balance on this thin element of thickness Ar during a small time interval At can be expressed as
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