\[ xyz = \text{constant} \]
The potential generated by an infinitely long charged wire is directly proportional to the natural logarithm of the distance from the wire. To determine the equipotential surface, the potentials from three such wires are superimposed.
Step 1: The potential contribution from each individual wire is a function of its perpendicular distance.
Step 2: An equipotential surface is defined as the locus of points where the sum of the potentials from all three wires remains constant.
Step 3: Analysis of the resultant potential expressions reveals that the relationship \( xy + yz + zx = constant} \) accurately defines the equipotential surface.
Two charges \( +q \) and \( -q \) are placed at points \( A \) and \( B \) respectively which are at a distance \( 2L \) apart. \( C \) is the midpoint of \( AB \). The work done in moving a charge \( +Q \) along the semicircle CSD (\( W_1 \)) and along the line CBD (\( W_2 \)) are 
Find work done in bringing charge q = 3nC from infinity to point A as shown in the figure : 