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Four electric charges +q, +q, -q and -q are placed at the corners of a square of side 2L (see figure). The electric potential at point A, mid-way between the two charges +q and +q, is

A

\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}(1+\frac{1}{\sqrt{5}})

B

\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}(1-\frac{1}{\sqrt{5}})

C

Zero

D

\frac{1}{4\pi\varepsilon_0}\frac{2q}{L}(1+\sqrt{5})

Step-by-Step Solution

  1. Identify Distances: Let the square of side 2L2L be arranged such that the two +q+q charges are at the top corners and the two q-q charges are at the bottom corners. Point A is the midpoint of the top side connecting the two +q+q charges.
  • Distance from A to each +q+q charge (r1r_1): Since A is the midpoint of the side of length 2L2L, r1=Lr_1 = L.
  • Distance from A to each q-q charge (r2r_2): Point A is separated horizontally by LL and vertically by 2L2L from the bottom corners. Using Pythagoras theorem, r2=L2+(2L)2=L2+4L2=5L2=L5r_2 = \sqrt{L^2 + (2L)^2} = \sqrt{L^2 + 4L^2} = \sqrt{5L^2} = L\sqrt{5}.
  1. Calculate Potential: The electric potential VV at a point due to a charge qq is V=14πε0qrV = \frac{1}{4\pi\varepsilon_0}\frac{q}{r} (Section 2.3). By the principle of superposition (Section 2.5), the total potential at A is the sum of potentials due to individual charges. VA=V(+q)+V(+q)+V(q)+V(q)V_A = V_{(+q)} + V_{(+q)} + V_{(-q)} + V_{(-q)} VA=14πε0(qL+qL+qL5+qL5)V_A = \frac{1}{4\pi\varepsilon_0} \left( \frac{q}{L} + \frac{q}{L} + \frac{-q}{L\sqrt{5}} + \frac{-q}{L\sqrt{5}} \right) VA=14πε0(2qL2qL5)V_A = \frac{1}{4\pi\varepsilon_0} \left( \frac{2q}{L} - \frac{2q}{L\sqrt{5}} \right) VA=14πε02qL(115)V_A = \frac{1}{4\pi\varepsilon_0} \frac{2q}{L} \left( 1 - \frac{1}{\sqrt{5}} \right)
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