Blundell Thermal Physics · Problem 10.4

The thermal diffusion equation

Physics — Statistical Mechanics · heat-fins-thermal-diffusion-rod

Problem

A microprocessor has an array of metal fins attached to it, whose purpose is to remove heat generated within the processor. Each fin may be represented by a long thin cylindrical copper rod with one end attached to the processor; heat received by the rod through this end is lost to the surroundings through its sides. Show that the temperature T(x,t)T(x,t) at location xx along the rod at time tt obeys the equation ρCp∂T∂t=κ∂2T∂x2−2aR(T),\rho C_p \frac{\partial T}{\partial t} = \kappa \frac{\partial^2 T}{\partial x^2} - \frac{2}{a} R(T), where aa is the radius of the rod, and R(T)R(T) is the rate of heat loss per unit area of surface at temperature TT. The surroundings of the rod are at temperature T0T_0. Assume that R(T)R(T) has the form of Newton's law of cooling, namely R(T)=A(T−T0).R(T) = A(T - T_0). In the steady state: (a) obtain an expression for TT as a function of xx for the case of an infinitely long rod whose hot end has temperature TmT_m; (b) show that the heat that can be transported away by a long rod (with radius aa) is proportional to a3/2a^{3/2}, provided that AA is independent of aa. In practice the rod is not infinitely long. What length does it need to have for the results above to be approximately valid? The radius of the rod, aa, is 1.5 1.5\,mm. [The thermal conductivity of copper is 380 W m−1 K−1380\,\mathrm{W\,m^{-1}\,K^{-1}}. The cooling constant A=250 W m−2 K−1A = 250\,\mathrm{W\,m^{-2}\,K^{-1}}.]

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