(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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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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