1. The problem statement, all variables and given/known data A long insulating cylinder has radius R, length l, and a non-uniform charge density per volume [tex]\rho = e^{ar}[/tex] where r is the distance from the axis of the cylinder. Find the electric field from the center of the axis for i) r < R ii) r > R 3. The attempt at a solution i) [tex]\oint \vec{E} \cdot d\vec{A} = \frac{\sum Q_{en}}{\epsilon_0}[/tex] [tex] \vec{E} 2\pi rl = \frac{\sum Q_{en}}{\epsilon_0}[/tex] So now here is the problem, if it is inside the cylinder I get something like (1) [tex]\rho V = Q[/tex] (2) [tex]\rho V' = Q_{en}[/tex] Divide them out and some algebra and I get [tex]Q\frac{V'}{V} = Q_{en}[/tex] Should I keep this? Does it even matter if it was a non-uniform density? I will stop here before I do ii...
[tex]V = \frac{4 \pi r^3}{3}[/tex] [tex]dV = 4\pi r^2 dr[/tex] [tex]\rho dV = e^{ar} 4\pi r^2 dr[/tex] Integrate that? This is just an indefinite integral right?
Oh wait, what am i doing lol [tex]V = \pi r^2 l [/tex] [tex]dV = 2\pi rl dr[/tex] [tex]\rho dV = e^{ar} 2\pi rl dr[/tex]
I had a feeling it was going to be a "0" to something What happens if [tex]\rho = \frac{1}{r}[/tex] What would the discontinuity mean? Would it mean that there is no Electric field in the line of its axis?
So anyways... [tex]2\pi l\int_{0}^{r} re^{ar} dr = 2\pi l \frac{e^{ar} (ar - 1) + 1}{a^2}[/tex] [tex]\vec{E} = \frac{1}{\epsilon_0 r}\frac{e^{ar} (ar - 1) + 1}{a^2}[/tex] So how do I tell the direction...? It looks all positive, it radiates outward?
Hi flyingpig! Such a distribution would mean you have infinite charge at the axis of the cylinder. That's not physically possible. You did not calculate the vector E, so you shouldn't write it down that way. You only calculated the component of E that is perpendicular to the surface that you integrated, which is the radial component. Furthermore you have assumed that it is the same everywhere on the surface of the cylinder. This is a reasonable assumption for a long cylinder with a symmetric distribution of charge. There are 2 more components to the E field at any point. Typically you would express them in cylindrical coordinates, meaning you have a component along the length of the cylinder, and a tangential component in the direction of the angle. Can you deduce what these components are? Which ratio?
Looks good. That's the charge. Good. (If you want to express it as a vector, include a unit vector to show the direction.) Yes. Assuming the charge is positive, the field points outward.
What happens if I say [tex]\rho(0) = c[/tex] and treat it as a piecewise function? [tex]\frac{Q_{en}}{Q_{charge\;of\;cylinder}}[/tex] [tex]\frac{\int \rho dV}{\rho V} = \frac{Q_{en}}{Q_{charge of cylinder}}[/tex] [tex]\frac{Q_{charge\;of\;cylinder}\int \rho dV}{\rho V} = Q_{en}[/tex] For [tex]\rhoV = e^{ar} 2\pi Rl[/tex] Where R is the radius of the cylinder
dV is proportional to r, so the effect of 1/r would be cancelled out when you integrate to find the charge.. Symmetry shows that there E=0 along the axis.
Well, with a function like 1/r the charge will still be near infinity if you get close enough to zero. Still physically impossible. Sorry. Errr... no, Gauss's formula for electric field and enclosed charge does not involve such a ratio.
Yeah it does, for an insulating surface with uniform density. I was thinking of [tex]\frac{Q_{charge\;of\;cylinder}\int \rho dV}{\rho V} = \frac{Q_{charge\;of\;cylinder}2\pi l \frac{e^{ar} (ar - 1) + 1}{a^2}}{e^{ar} \pi R^2 l}= Q_{en}[/tex]