Diffusion Equation Invariant to Linear Temp. Transform

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Discussion Overview

The discussion revolves around the invariance of the diffusion equation under a linear transformation in the temperature field, specifically the transformation defined as $\overline{T} = \alpha T + \beta$. Participants explore the implications of this transformation on the diffusion equation and its solutions.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Homework-related

Main Points Raised

  • One participant presents the transformation and derives the modified diffusion equation, questioning if the substitution is correct.
  • Another participant agrees with the derivation, noting that the set of solutions forms a vector space that includes constant functions.
  • A participant expresses skepticism about the simplicity of the problem, suggesting it may be too straightforward.
  • Another participant acknowledges the simplicity but highlights a deeper meaning, indicating that given one solution, a second can be constructed using the transformation.
  • A further suggestion is made to consider the invariance of the PDE under a different change of variables involving time and space scaling.
  • Participants question the practical utility of the invariance discussed.

Areas of Agreement / Disagreement

Participants generally agree on the correctness of the transformation and its implications for the solutions of the diffusion equation. However, there is some disagreement regarding the perceived simplicity of the problem and its significance.

Contextual Notes

Some assumptions regarding the nature of the solutions and the context of the problem may not be fully articulated, leaving room for further exploration of the implications of the transformation.

Who May Find This Useful

This discussion may be useful for students and educators in physics or mathematics, particularly those interested in differential equations and their applications in heat diffusion problems.

Dustinsfl
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Show the diffusion equation is invariant to a linear transformation in the temperature field
$$
\overline{T} = \alpha T + \beta
$$
Since $\overline{T} = \alpha T + \beta$, the partial derivatives are
\begin{alignat*}{3}
\overline{T}_t & = & \alpha T_t\\
\overline{T}_{xx} & = & \alpha T_{xx}
\end{alignat*}
So $T_t = \frac{1}{\alpha}\overline{T}_t$ and $T_{xx} = \frac{1}{\alpha}\overline{T}_{xx}$.
The diffusion equation is
$$
\frac{1}{\alpha}T_t = T_{xx}.
$$
By substitution, we obtain
$$
\frac{1}{\alpha}\overline{T}_t = \overline{T}_{xx}.
$$
Correct?
 
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Yes, as the set of solutions of such an equation is a vector space which contains constant functions.
 
girdav said:
Yes, as the set of solutions of such an equation is a vector space which contains constant functions.

So that is all that it was? It seems to simple.
 
It may be for example the first question of a homework or a test, so it's not necessarily difficult. (maybe maybe the other question can be harder)
 
dwsmith said:
So that is all that it was? It seems to simple.
Yes, it may be simple (in this case) but there's a deeper meaning. It means, given one solution $T_0$, you can construct a second solution $T = \alpha T_0 + \beta$.

You might also want to check that this same PDE is invariant under the change of variables

$\bar{t} = k^2 t,\;\;\; \bar{x} = k x$

i.e.

$ T_{\bar{t}}=\alpha T_{\bar{x} \bar{x}} \;\; \implies \;\; T_t = \alpha T_{xx}$.

The next question $-$ how is this useful?
 

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