Charge Distribution - Equilibrium Points

Consider the following static volumetric charge density profile:

ρ ( r ) = 1 10 + ( r 1 ) 2 0 r < \rho (r) = - \frac{1}{10} + (r - 1)^2 \\ 0 \leq r < \infty

In the above, r r is the distance from the origin in three-dimensional space. Suppose a positive test charge is placed at radial position r r , and that the charge begins at rest but is free to move under the influence of the electric field.

There is one stable equilibrium radius r S r_S , and two unstable equilibrium radii r U 1 r_{U1} and r U 2 r_{U2} .

Determine the following ratio: r S r U 1 + r U 2 \large{\frac{r_S}{r_{U1} + r_{U2}}}


The answer is 0.6666.

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1 solution

Otto Bretscher
Dec 4, 2018

Up to a constant, the potential Φ \Phi is given by Poisson's equation 2 Φ = ρ \nabla^2\Phi=\rho . Since everything depends on r r alone, we need to solve the equation 1 r 2 d d r ( r 2 ( d Φ d r ) ) \frac{1}{r^2}\frac{d}{dr}\left(r^2\left(\frac{d\Phi}{dr}\right)\right) = r 2 2 r + 9 10 =r^2-2r+\frac{9}{10} , which gives d Φ d r = r 3 5 r 2 2 + 3 r 10 \frac{d\Phi}{dr}=\frac{r^3}{5}-\frac{r^2}{2}+\frac{3r}{10} . The equilibria d Φ d r = 0 \frac{d\Phi}{dr}=0 are at r = 0 , 1.5 r=0, 1.5 and 1 1 , with the last one being stable, and the answer is 1 0 + 1.5 0.667 \frac{1}{0+1.5}\approx \boxed{0.667} .

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