A few conceptual questions about a charged sphere inside an initially neutral spherical shell and about uniform E for a charged plane.
How would I go about calculating potential at a certain point in space without a potential value at a reference point? I know that there is a constant added on if you do an indefinite integral right from the start to find $V(X)$, but how does this relate to this situation? I'm mainly confused on the difference between finding delta v and v through integration.
I know that $\Delta V$ = $\int_a^x \! E \, \mathrm{d}x$ where $x$ is the point I'm trying to calculate the potential at and a is the reference point. $\Delta V = V(x)-v(a)$. So, for the sake of a shorter equation, I assume that $E$ is uniform and in this example is for a surface: $E = \sigma/ \epsilon_0$. If I substitute this into the $\delta V$ equation and evaluate the 'definite' integral I get $V(x)-V(a) = -(\sigma/\epsilon_0 x-\sigma/\epsilon_0 a)$. I am looking for $V(X)$ so I add $V(A)$ to the other side of the equation but it doesn't cancel with anything and i'm left with 2 times the potential at the reference point. Why?
Assuming that a charged sphere is inside a neutral spherical shell. How would I go about finding the potential at a radius that is between the inner sphere and the inner surface of the spherical shell. I know that the potential for a point charge is $kq/r - kq/a$ where $a$ is the reference point, usually set at x$ = \infty$ since that is where $V=0$. But I can't use this reference point at this radius. So how would I find the potential here?