To determine the electric potentials at the four points due to the charges, we need to consider how electric potential (V) due to a point charge is defined:
\[ V = k \frac{Q}{r} \]
Where:
- \(V\) is the electric potential.
- \(k\) is Coulomb's constant.
- \(Q\) is the charge.
- \(r\) is the distance from the charge to the point of interest.
Analyzing Each Point:
-
Point A (Top Left Corner):
- Distance from charge \(Q\) (bottom left corner) is \(d\).
- Distance from charge \(2Q\) (bottom right corner) is \(\sqrt{2}d\).
- Potential \(V_A = k \frac{Q}{d} + k \frac{2Q}{\sqrt{2}d} = k\frac{Q}{d} + k\frac{2Q}{\sqrt{2}d}\).
-
Point B (Top Right Corner):
- Distance from charge \(Q\) (bottom left corner) is \(\sqrt{2}d\).
- Distance from charge \(2Q\) (bottom right corner) is \(d\).
- Potential \(V_B = k \frac{Q}{\sqrt{2}d} + k \frac{2Q}{d} = k\frac{Q}{\sqrt{2}d} + k\frac{2Q}{d}\).
-
Point C (Center of Square):
- Distance from charge \(Q\) (bottom left corner) is \(\frac{\sqrt{2}}{2}d\).
- Distance from charge \(2Q\) (bottom right corner) is also \(\frac{\sqrt{2}}{2}d\).
- Potential \(V_C = k \frac{Q}{\frac{\sqrt{2}}{2}d} + k \frac{2Q}{\frac{\sqrt{2}}{2}d} = k\frac{Q \sqrt{2}}{d} + k\frac{2Q \sqrt{2}}{d} = k\frac{3Q\sqrt{2}}{d}\).
-
Point D (Centered on Bottom Edge):
- Distance from charge \(Q\) (bottom left corner) is \(\frac{d}{2}\).
- Distance from charge \(2Q\) (bottom right corner) is also \(\frac{d}{2}\).
- Potential \(V_D = k \frac{Q}{\frac{d}{2}} + k \frac{2Q}{\frac{d}{2}} = k\frac{2Q}{d} + k\frac{4Q}{d} = k\frac{6Q}{d}\).
Summary of Potentials:
- \(V_A = k \left( \frac{Q}{d} + \frac{2Q}{\sqrt{2}d} \right)\)
- \(V_B = k \left( \frac{Q}{\sqrt{2}d} + \frac{2Q}{d} \right)\)
- \(V_C = k \frac{3Q\sqrt{2}}{d}\)
- \(V_D = k \frac{6Q}{d}\)
Comparison:
- \(V_D\) is the largest due to the maximum contributions from both charges.
- \(V_C\) follows, as it has the sum of potentials from both charges at equal distances.
- \(V_A\) and \(V_B\) are more complicated; however, generally we can compare:
- Since both \(Q\) and \(2Q\) contribute to \(V_A\) and \(V_B\) but differ in distance to the charges, \(V_A < V_B\).
Thus, we can rank the potentials from largest to smallest as follows:
\[ V_D > V_C > V_B > V_A \]