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Mathematics LibreTexts

10.1: Temperature on a Disk

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Let us now turn to a different two-dimensional problem. A circular disk is prepared in such a way that its initial temperature is radially symmetric, u(ρ,ϕ,t=0)=f(ρ). Then it is placed between two perfect insulators and its circumference is connected to a freezer that keeps it at 0 C, as sketched in Fig. 10.1.2.

A circular plate, insulated from above and below.

Figure 10.1.1: A circular plate, insulated from above and below.

Since the initial conditions do not depend on ϕ, we expect the solution to be radially symmetric as well, u(ρ,t), which satisfies the equation ut=k[2uρ2+1ρuρ],u(c,t)=0,u(ρ,0)=f(ρ).

The initial temperature in the disk.

Figure 10.1.2: The initial temperature in the disk.

Once again we separate variables, u(ρ,t)=R(ρ)T(t), which leads to the equation

1kTT=R+1ρRR=λ. This corresponds to the two equations

ρ2R+ρR+λρ2R=0,R(c)=0mT+λkT=0.

The radial equation (which has a regular singular point at ρ=0) is closely related to one of the most important equation of mathematical physics, Bessel’s equation. This equation can be reached from the substitution ρ=x/λ, so that with R(r)=X(x) we get the equation

x2d2dx2X(x)+xddxX(x)+x2X(x)=0,X(λc)=0.


This page titled 10.1: Temperature on a Disk is shared under a CC BY-NC-SA 2.0 license and was authored, remixed, and/or curated by Niels Walet via source content that was edited to the style and standards of the LibreTexts platform.

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