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Question: Four electric charges +q, +q, -q and -q are placed in order at the corners of a square of side 2 L. ...

Four electric charges +q, +q, -q and -q are placed in order at the corners of a square of side 2 L. The electric potential at point midway between the two positive charges is

A

14πE02qL(1+15)\frac{1}{4\pi E_0} \frac{2q}{L} (1 + \frac{1}{\sqrt{5}})

B

14πE02qL(115)\frac{1}{4\pi E_0} \frac{2q}{L} (1 - \frac{1}{\sqrt{5}})

C

14πE02qL(15)\frac{1}{4\pi E_0} \frac{2q}{L} (1 - \sqrt{5})

D

14πE02qL(1+5)\frac{1}{4\pi E_0} \frac{2q}{L} (1 + \sqrt{5})

Answer

14πE02qL(115)\frac{1}{4\pi E_0} \frac{2q}{L} (1 - \frac{1}{\sqrt{5}})

Explanation

Solution

The electric potential at a point due to a point charge is given by:

V=14πϵ0qrV = \frac{1}{4\pi\epsilon_0} \frac{q}{r}

Where:

  • VV is the electric potential
  • qq is the charge
  • rr is the distance from the charge to the point
  1. Distances:

    • The two +q charges are at a distance LL from the midpoint.
    • The two -q charges are at a distance L2+(2L)2=5L\sqrt{L^2 + (2L)^2} = \sqrt{5}L from the midpoint.
  2. Individual Potentials:

    • Potential due to each +q charge: V+=14πϵ0qLV_+ = \frac{1}{4\pi\epsilon_0} \frac{q}{L}
    • Potential due to each -q charge: V=14πϵ0q5LV_- = -\frac{1}{4\pi\epsilon_0} \frac{q}{\sqrt{5}L}
  3. Total Potential: The total potential VV is the sum of the potentials due to all charges:

    V=2V++2V=2(14πϵ0qL)+2(14πϵ0q5L)V = 2V_+ + 2V_- = 2\left(\frac{1}{4\pi\epsilon_0} \frac{q}{L}\right) + 2\left(-\frac{1}{4\pi\epsilon_0} \frac{q}{\sqrt{5}L}\right)

    V=14πϵ02qL(115)V = \frac{1}{4\pi\epsilon_0} \frac{2q}{L} \left(1 - \frac{1}{\sqrt{5}}\right)