Diffusion of energy by heat flow

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SUMMARY

The discussion focuses on deriving the diffusion equation for energy by heat flow, specifically from the heat flow equation in one dimension, represented as $$ j_H=-\kappa \partial_x T $$, where ## \kappa ## is thermal conductivity. The second equation $$ \partial_t T=D_H \partial^2_x T $$ is established, with ## D_H ## dependent on thermal conductivity ## \kappa ##, heat capacity ## C ##, and density ## \rho ##. The participants emphasize the need to manipulate the equations correctly without assuming the second equation in the proof process.

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  • Understanding of heat flow equations and thermal conductivity
  • Familiarity with partial derivatives and their applications in physics
  • Knowledge of energy density concepts, specifically internal energy per unit volume
  • Basic principles of calculus, particularly Taylor series expansion
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Nacho Verdugo
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Homework Statement


This problem belongs to the Intermediate Physics for Medicine and Biology, Hobbie Chapter 4.

The heat flow equation in one dimension

$$ j_H=-\kappa \partial_x T $$

where ## \kappa ## is the termal conductivity in ## Wm^{-1}K^{-1}##. One often finds an equation for the diffusion of energy by heat flow:

$$ \partial_t T=D_H \partial^2_x T $$

The units of ## j_H## are ## Jm^{-2}s^{-1}##. The internal energy per unit volumen is given by ##u=\rho CT##, where C is the heat capacity per unit mass and ##\rho## is the density of the material. Derive the second equation from the first and show ## D_H ## depends on ## \kappa, C## and ##\rho##.

Homework Equations

The Attempt at a Solution


[/B]
I tried this:

As ## u=\rho CT ##, I can write the temperature as ##T=\frac{u}{C\rho}##, so in the first equation:

$$ j_H=-\kappa \partial_x \left( \frac{u}{C\rho} \right) $$

and rewriting this and replacing it in the second equation:

$$\partial_t T=D_H\partial_x(j_H/\kappa) $$

which is similar to

$$\partial_t T=D_H \partial_x \partial_x ({u}{C\rho}) $$

but I got stucked here because I can't derivate this. Any ideas on how to move on?
 
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Nacho Verdugo said:
rewriting this and replacing it in the second equation:
The second equation is the thing to be proved, no? So you cannot use it in the proof.
Consider a small element at position x length dx, temperature T(x,t). Neighbouring elements are at temperatures T(x-dx, t) and T(x+dx, t).
What is the heat flow into the element from each neighbour? Approximate T(x-dx, t) etc. using the usual f(x+dx)=f(x)+f'(x)dx+ ... rule, but taking into account the second order terms.
 

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