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(1) Show that Fourier's law can be written (for constant pCp) as d dy (PCT) for one-dimensional heat flow. In addition, show that Newton's qy = law, for constant p, can be written as: Tyx = -V- v dyr (pvx) (pv₂) Discuss the analogies between the fluxes, constants and the gradients as they appear in these equations.

(1) Show that Fourier's law can be written (for constant pCp) as d dy (PCT) for one-dimensional heat flow. In addition, show that Newton's qy = law, for constant p, can be written as: Tyx = -V- v dyr (pvx) (pv₂) Discuss the analogies between the fluxes, constants and the gradients as they appear in these equations.

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(1) Show that Fourier's law can be written (for constant pCp) as d 9y = -a dy (oG,T) for one-dimensional heat flow. In addition, show that Newton's law, for constant p, can be written as: d Tyx = -v dy Discuss the analogies between the fluxes, constants and the gradients as they appear (*aの) in these equations.
Transcribed Image Text:(1) Show that Fourier's law can be written (for constant pCp) as d 9y = -a dy (oG,T) for one-dimensional heat flow. In addition, show that Newton's law, for constant p, can be written as: d Tyx = -v dy Discuss the analogies between the fluxes, constants and the gradients as they appear (*aの) in these equations.
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