V = \frac{1}{4\pi\epsilon_{0}}∫^{2\pi}_{0}d\phi∫^{\pi}_{0}sin\thetad\theta∫^{R}_{0} \frac{ρ_{0}r^{2}}{r} r^{2}dr
Solving this:
V= \frac{ρ_{0}R^{4}}{4\epsilon_{0}}
I'm quite happy with this answer, but if it is incorrect please let me know.
Thanks for the help
Homework Statement
Solid ball of charge with radius R and volume charge density ρ(r) = ρ0r2, centred at the origin.
I have already found the electric field for r<R and r>R and also the potential at the origin by using the formula:
V = -∫E.dl
Now i want to find the potential at the...