How can the heat equation be derived for a long circular cylinder?

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SUMMARY

The heat equation for a long circular cylinder can be derived by applying the three-dimensional heat equation and transforming it into cylindrical coordinates. The temperature distribution is expressed as a function of time (t) and the radial distance (r) from the cylinder's axis, where r is defined as r = √(x² + y²). The derivation involves rewriting the heat equation in spherical coordinates to utilize the symmetry of the cylinder, leading to the equation u_{t} = k(u_{rr} + (u_{r}/r)).

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Consider heat flow in a long circular cylinder where the temperature depends only on t and on the distance r to the axis of the cylinder. Here r=\sqrt{x^{2}+y^{2}} is the cylindrical coordinate. From the three dimensional heat equation derive the equation u_{t}=k(u_{rr}+\frac{u_{r}}{r}).

My book describes how the general heat equation is derived, but I'm having trouble incorporating the equation for r and in general understanding these concepts.

The book starts out with:

H(t)=\int\int\int c\rho u dxdydz which I'm somewhat confident I can change to

H(t)=\int\int\int c\rho u dxdydr because of the equation with r

Then the book has
\frac{dH}{dt}=\int\int\int c\rho u_{t} dxdydr which makes sense to me

then after this I am a bit confused. I don't really know what to do next in terms of answering the question.
 
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This can be done very easily, by rewriting the heat equation in spherical coordinates and taking advantage of the symmetry of the situation. A little bit of re-arranging gives you the equation.
 

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