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NEET PHYSICSEasy

An electric dipole is placed as shown in the figure. The electric potential (in 10² V) at the point P due to the dipole is: (ε₀ = permittivity of free space and 1/4\pi ε₀ = k)

A

(8/3) qk

B

(3/8) qk

C

(5/8) qk

D

(8/5) qk

Step-by-Step Solution

  1. Principle of Superposition: The electric potential (VV) at any point due to a system of charges is the algebraic sum of the potentials due to the individual charges. For a dipole consisting of charges +q+q and q-q, the potential at point P is given by: VP=V+q+Vq=kqr1+kqr2=kq(1r11r2)V_P = V_{+q} + V_{-q} = k \frac{q}{r_1} + k \frac{-q}{r_2} = kq \left( \frac{1}{r_1} - \frac{1}{r_2} \right), where r1r_1 and r2r_2 are the distances of point P from +q+q and q-q respectively.
  2. Analysis of Probable Answer: The correct option is given as 38qk\frac{3}{8}qk. This implies that the geometric factor (1r11r2)\left( \frac{1}{r_1} - \frac{1}{r_2} \right) must equal 38\frac{3}{8}.
  3. Hypothetical Geometry: For example, if the distance from +q+q to P is 2 units (r1=2r_1 = 2) and from q-q to P is 8 units (r2=8r_2 = 8), then 1218=4818=38\frac{1}{2} - \frac{1}{8} = \frac{4}{8} - \frac{1}{8} = \frac{3}{8}. Without the figure, the exact distances cannot be verified, but the method remains the scalar addition of potentials.
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