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6.4 Show that Fourier's law can be written (for constant Cp ) as qy=dyd(CpT) for one-dimensional heat flow. In addition, show that Newton's law, for
6.4 Show that Fourier's law can be written (for constant Cp ) as qy=dyd(CpT) for one-dimensional heat flow. In addition, show that Newton's law, for constant , is yx=vddyd(vx). Discuss the analogies between the fluxes, constants, and gradients as they appear in these equations
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