Transcription of STEADY HEAT CONDUCTION
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STEADY heat CONDUCTIONIn heat transfer analysis, we are often interested in the rate of heat transferthrough a medium under STEADY conditions and surface temperatures. Suchproblems can be solved easily without involving any differential equationsby the introduction of the thermal resistance conceptin an analogous mannerto electrical circuit problems. In this case, the thermal resistance correspondsto electrical resistance, temperature difference corresponds to voltage, and theheat transfer rate corresponds to electric start this chapter with one-dimensional STEADY heat conductionin aplane wall, a cylinder, and a sphere, and develop relations for thermal resis-tancesin these geometries.
where R conv (K/W) (3–8) is the thermal resistanceof the surface against heat convection, or simply the convection resistanceof the surface (Fig. 3–4).Note that when the convec-tion heat transfer coefficient is very large (h → ), the convection resistancebecomes zero and T s T.That is, the surface offers no resistance to convec- tion, and thus it does not slow down the heat …
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