An aluminium cold plate (mass

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Vector calculus and field geometry · Partial differential equations and boundary-value problems

Conditions of Validity, Ch Gauss, Stokes and Green proved, and the first inversion of a differential operator

Problem

An aluminium cold plate (mass m=1.2 kgm=1.2\,\mathrm{kg}, specific heat capacity cp=900 J kg−1 K−1c_p=900\,\mathrm{J\,kg^{-1}\,K^{-1}}) is a rectangular slab used to cool electronics mounted on its top face. The mounted chips dissipate a steady total power P=50 WP=50\,\mathrm W inside the plate, distributed however the manufacturer likes. Four side faces and the top face are thermally insulated; the bottom face, of area A=0.030 m2A=0.030\,\mathrm m^2, is cooled by a coolant loop that, once running has settled, removes a measured uniform outward heat flux q=1400 W m−2q=1400\,\mathrm{W\,m^{-2}} over that face. ((a)) Steady conduction inside the plate obeys ∇2u=−f/k\nabla^2u=-f/k for internal heat-source density ff and conductivity kk, with outward heat-flux vector q=−k∇u\mathbf q=-k\nabla u. Using Green's first identity with ϕ=1\phi=1, ψ=u\psi=u, show that a steady state can exist only if ∮∂Vq⋅n^ dS=P,\oint_{\partial V}\mathbf q\cdot\hat{\mathbf n}\,\mathrm dS = P, i.e. the total heat leaving through the whole boundary must equal the total power generated inside, whatever the (unknown) distribution of ff or of the boundary flux. ((b)) Decide whether the cold plate is in a steady state with the measured coolant flux, and if it is not, find the rate of change of the plate's mean temperature, treating the plate as a lumped mass of uniform temperature.

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