A diamond anvil in a high-pressure cell has a lower-grade conductivity than the…

PHYSICS · Multi-part · Fermi University Physics · Condensed Matter, Materials & Soft Matter · Lattice dynamics and thermal properties of solids · Lattice dynamics and thermal properties of solids

Condensed Matter Physics, Ch Thermal expansion and lattice thermal conductivity

Problem

A diamond anvil in a high-pressure cell has a lower-grade conductivity than the purest bulk diamond, κ=1500 W m−1K−1\kappa = 1500\,\mathrm{W\,m^{-1}K^{-1}} at 300 K300\,\mathrm{K}, with cV=1.8×106 J m−3K−1c_V = 1.8\times10^6\,\mathrm{J\,m^{-3}K^{-1}}, v=1.3×104 m s−1v = 1.3\times10^4\,\mathrm{m\,s^{-1}} and a=3.57 A˚a = 3.57\,\mathrm{\mathring{A}} as for bulk diamond. ((a)) Estimate its phonon mean free path, in nanometres and in lattice constants. ((b)) The anvil is t=1.5 mmt = 1.5\,\mathrm{mm} thick and carries Q=2.0 WQ = 2.0\,\mathrm{W} of heat away from the sample through a cross-sectional area A=0.50 mm2A = 0.50\,\mathrm{mm^2}. Using the definition of thermal conductivity, Jx=−κ dT/dxJ_x = -\kappa\,\mathrm{d}T/\mathrm{d}x, in steady state with a uniform gradient, estimate the temperature difference across the anvil's thickness.

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