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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:

  1. Two charges \(+Q\) and \(+Q\) are placed on a line at \(z=+D\) and \(z=-D\text{,}\) respectively.

  2. Two charges \(+Q\) and \(-Q\) are placed on a line at \(z=+D\) and \(z=-D\text{,}\) respectively.

Hint.

You may be tempted to use the iconic equation for the electrostatic potential to give an answer along the lines of

\begin{equation*} V=k\left(\frac{q_1}{r_1}+\frac{q_2}{r_2}\right) \end{equation*}

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.

Hint.

In some cases, the contributions from the two terms cancel. How does this cancellation relate to the symmetries of the problem?