Practice portal › Thermal Properties of Matter › Conduction and Thermal Resistance
Asked in AIEEE 2005 · Radial conduction through shells
Idea: integrate the resistance outward, because the conducting area 4π r² changes with radius.
R=∫_r₁^r₂(dr)/(4π Kr²)=(r₂-r₁)/(4π Kr₁r₂).
(dQ)/(dt)=(T₁-T₂)/R=(4π Kr₁r₂(T₁-T₂))/(r₂-r₁).
With K and the temperature difference fixed, the geometry enters only through (r₁r₂)/(r₂-r₁).
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