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I am learning Mean value property (MVP) of the heat equation. MVP of Laplace equation was relatively easy to understand I think it is because of the spherical symmetry. But I am not able to appreciate the MVP of heat equation. It's not very easy to imagine the "heat ball" in the following theorem from a note:

enter image description here

Here are questions:

  • How do I define a heat ball?
  • How does it actually look like?
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  • $\begingroup$ What is your question? $\endgroup$
    – user31373
    Jun 22, 2012 at 15:09
  • $\begingroup$ @LeonidKovalev : My question is how do i define a heat ball ? And how does it actually look like ? $\endgroup$
    – Theorem
    Jun 22, 2012 at 15:26
  • $\begingroup$ Could you give a reference to a text you are reading? $\endgroup$
    – abatkai
    Jun 22, 2012 at 15:31
  • $\begingroup$ @abatkai : I have added the reference . Thank you $\endgroup$
    – Theorem
    Jun 22, 2012 at 15:40

2 Answers 2

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The "heat ball" is defined as it is in the note you cited which is bases on Evans's Partial Differential Equations Chapter 2.3.

For fixed $x\in{\bf R}^n$, $t\in{\bf R}$ and $r>0$, we define $$ E(x,t;r)=\left\{(y,s)\in {\bf R}^{n+1}\bigg|\; s\leqslant t,\ \dfrac{1}{(4\pi(t-s))^{n/2}}\exp\left({-\dfrac{|x-y|^2}{4(t-s)}}\right)\geqslant\frac{1}{r^n}\right\}. $$

The Wikipedia article Mean-value property for the heat equation also gives a similar definition.


Note that in the definition, one should replace $s\leqslant t$ with $s<t$. To get some ideas of what such "ball" would look like, consider $n=1$ and $$ E(0,0;1)=\left\{(y,s)\in {\bf R}^{2}\bigg|\; s<0,\ \dfrac{1}{(4\pi(-s))^{1/2}}\exp\left({-\dfrac{|-y|^2}{4(-s)}}\right)\geqslant 1\right\}\\ =\left\{(y,s)\in{\bf R}^2\bigg|\; 0<-s\leqslant\frac{1}{4\pi}, y^2\leq 2s\log(-4\pi s)\right\} $$ To get $-s\leqslant\frac{1}{4\pi}$ one can simply observe that $\exp\left(-\dfrac{|-y|^2}{4(-s)}\right)\leqslant 1$ for $s<0$ and thus $$ \sqrt{-4\pi s}\leqslant 1. $$ On the other hand, taking the logarithm of $\dfrac{1}{(4\pi(-s))^{1/2}}\exp\left({-\dfrac{|-y|^2}{4(-s)}}\right)\geqslant 1$ gives $$ y^2\leq 2s\log(-4\pi s). $$

The boundary of the heat ball is like this:

enter image description here

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  • $\begingroup$ How did you derive the expression for $E(0,0; 1)$? If you assume $t = 0$, shouldn't $s$ be less than $0$? $\endgroup$
    – el_tenedor
    Sep 14, 2016 at 7:05
  • $\begingroup$ @el_tenedor: Thanks for pointing that out! That's certainly a mistake and I have now edited the answer. $\endgroup$
    – user9464
    Aug 11, 2017 at 0:48
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    $\begingroup$ I have just noticed that I'm responding to a comment about one year old. $\endgroup$
    – user9464
    Aug 11, 2017 at 0:55
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There is an illustration on page 53 of PDE by Evans. Nothing mysterious, just an ellipsoid-like shape with the "center" $(x,t)$ located at the center on the top boundary (not in the interior, as for elliptic PDE).

The definition is in the book you are reading, formula (23).

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  • $\begingroup$ Sir, Why should it be ellipsoid ? Can you help me to understand it $\endgroup$
    – Theorem
    Jun 22, 2012 at 18:07
  • $\begingroup$ @Theorem For each fixed value of time variable $s$, you get a two-dimensional slice which is a circle. The radius of the circle depends on $s$: it drops to zero when $s=t$ and when $s$ is much smaller than $t$. $\endgroup$
    – user31373
    Jun 22, 2012 at 18:35

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