A stationary charge of -31.04 `microC is located at the origin, and a charge of -94.1 `microC is located at the point ( .32 m,0,0).
We find the force exerted on the moveable charge at each of the two points, and use these forces to estimate the average force:
Assuming this to be the average force on the charge over the interval between the points (it is not in fact equal to the average; it is higher than the average but the average gives us a reasonable approximation in this case), we find the work using this force and the displacement from the first point to the second.
As a charge q2 is moved from distance r1 = x1 to distance r2 = x2 from a fixed charge q1, the force on the charge changes from F1 = k q1 q2 / r1^2 to F2 = k q1 q2 / r2^2.
This change is not linear, so the average force exerted is not exactly equal to the average of F1 and F2; however if the forces are not too different the average of the forces gives a reasonable approximation of the average force.
Using (F1 + F2) / 2 as the approximate average force, we obtain an estimate of the work done when we multiply the force opposite to this average force by the displacement `dr = r2 - r1= x2 - x1 to obtain
approximate W = -(F1 + F2) / 2 * (r2 - r1) = -(F1 + F2) / 2 * (x2 - x1).
The figure shows the charge q2 at positions (x1,0) and (x2,0), and the forces F1 and F2 at those points (assuming a force of attraction; if the charges are of the same sign the forces will be forces of repulsion). The force required to move the charge from x1 to x2 will be in the direction opposite to F1 and F2. If we use (F1 + F2) / 2 as the approximate average force over the interval, we must therefore apply an approximate average force of -(F1 + F2) / 2 over distance (x2 - x1), obtaining the indicated work.
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