Section 4.5 Two Point Charges
Start by writing down a formula for the electrostatic potential \(V(\rr)=V(x,y,z)\) everywhere in space due to a single point charge that is not located at the origin. Then:
Activity 4.5.1.
Find the electrostatic potential everywhere in space for the following two cases:
Two charges \(+Q\) and \(+Q\) are placed on a line at \(z=+D\) and \(z=-D\text{,}\) respectively.
Two charges \(+Q\) and \(-Q\) are placed on a line at \(z=+D\) and \(z=-D\text{,}\) respectively.
You may be tempted to use the iconic equation for the electrostatic potential to give an answer along the lines of
But this expression doesn't provide enough information to describe \(r_1\) and \(r_2\text{.}\) This is a good example of the need to “unpack” the iconic equation. Your final answers should explicitly involve \(x,y,z\) and \(D\text{.}\)
Activity 4.5.2.
Simplify your expressions, assuming that you are evaluating the potential along the \(z\)-axis. Then do the same, this time assuming you are on the \(x\)-axis.
In some cases, the contributions from the two terms cancel. How does this cancellation relate to the symmetries of the problem?