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I am looking for a reference where the following situation or something similar could have been studied. As a foreword, my question may not be very technical since I am from an engineering background. I have tried to provide an intuitive explanation of the problem. I am also looking for a mildly technical reference or answer:

Heat equation can be used to study diffusion of heat on a surface. On a plane the boundary for a such a heat equation is a circle. I am looking for a system of three heat equation type PDEs (call them $a_{1}$, $a_{2}$ and $a_{3}$) so that some conditions are satisfied.

1) $a_{1}$, $a_{2}$ and $a_{3}$ describe propagation of heat starting at three different points $A_{1}$, $A_{2}$ and $A_{3}$ on the plane.

2) Stopping time of $a_{i}$ is when intersection of boundary of $a_{i}$ and union of boundaries $a_{j}$ and $a_{k}$ is non empty with $i \ne j \ne k \ne i$ $\forall i \in \{1,2,3\}$.

Let the stopping time of $a_{i}$ be $t_{i}$. After giving a simple description of pdes that could satisfy the above conditions, I also need to find expressions for $t_{i}$ which is what I am truly after since it finding $t_{i}$ could provide distance between $A_{i}$ to it closest neighbor without using the euclidean formula. Can one get the PDE to stop diffusing without introducing an artificial stopping time? Can one generalize this to many points in $n$-dimensions (real or complex). Such a system could capture closest neighbors to each given point.

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  • $\begingroup$ When you say "the boundary for a such a heat equation is a circle" do you mean the level sets for a fundamental solution are circles? $\endgroup$
    – S. Carnahan
    Apr 25, 2011 at 4:15
  • $\begingroup$ I think that is what I am implying. $\endgroup$
    – Turbo
    Apr 25, 2011 at 5:46

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This answer makes some assumptions about what the OP is asking. In particular I am using Scott's interpretation that the boundaries of interest correspond to level sets of the fundamental solution.

I suppose you have to specify which level set you are talking about. Since the heat equation has infinite propagation speed, you can make the $t_i$ as close to zero as you like by looking at level sets $a_i = \epsilon$ for $\epsilon$ sufficiently small. If you fix $\epsilon$ (or $\epsilon_i$) then you are looking at a collection of three circles in the plane with radius $r_i(t) = \left(4kt \log(1/\epsilon) + 2kt \log(4 \pi k t)\right)^\frac{1}{2}$ (assuming the standard heat equation with diffusion constant k) and you are asking when these circles intersect. The circle about $A_i$ will intersect the circle about $A_j$ when $r_i + r_j \ge |A_i - A_j|$.

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  • $\begingroup$ Hi Aaron: Thank you for the answer. Can you write explicitly the system of PDEs that will start diffusing and stop at the closest neighbor's level set? $\endgroup$
    – Turbo
    Apr 26, 2011 at 1:54
  • $\begingroup$ I am wondering what the system would look like for more than $3$ points in $n \ge 3$ dimensions. $\endgroup$
    – Turbo
    Apr 26, 2011 at 1:55
  • $\begingroup$ Caveat: Maybe I'm not understanding your question. I am imagining $u_t = D\Delta u$ where $u(x,t) \in \R^m$ and $x \in \R^n$ and $D$ is a diagonal matrix with entries $k_i$. This is just a collection of uncoupled heat equations in $\R^n$ whose fundamental solution is just a vector of Gaussians. It sounds like the solution that you are interested in corresponds to $u_i$ a Gaussian centered at $A_i$. The stopping time is introduced artificially by picking levels $\epsilon_i$ and taking logarithms of the Gaussians to solve for the radius of the spherical level set as a function of time ... $\endgroup$ Apr 26, 2011 at 2:24
  • $\begingroup$ (continued) ... and then call a collision any time that $|A_i - A_j| \ge r_i + r_j$. Getting the PDE to stop diffusing without introducing an artificial stopping time would be more subtle. $\endgroup$ Apr 26, 2011 at 2:27
  • $\begingroup$ "Getting the PDE to stop diffusing without introducing an artificial stopping time would be more subtle." Actually I think I am interested in exactly this "automation" of the stopping times so that the description of the PDEs themselves would capture the closest neighbors. Such a description could provide an analytical gadget to some euclidean graph problems $\endgroup$
    – Turbo
    Apr 26, 2011 at 2:46

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