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Future, you would utilize this boundary situation and address for Fourier's 2nd Regulation to obtain the internal temperature distribution. Assuming no interior warmth technology, the solution is ρ C p ( ∂ T ∂ t + v → ▽ T ) = k ▽ T displaystyle rho C_ p ( partial T more than partial t + overrightarrow v bigtriangledown T)=kbigtriangledow