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MHT CET 202621 AprilMorning Shift
Exam
MHT CET
Year
2026
Date
21 April
Shift
Morning Shift
Subject
Physics
Chapter
Electrostatics

MHT CET 2026 · 21 April · Morning Shift · Physics · Electrostatics

The electric potential due to a dipole at point P making an angle...

The electric potential due to a dipole at point P making an angle 120^{}^{\circ} with the axis of a dipole is
(\varepsilon_0=permitivityoffreespace,= permitivity of free space,p=electricdipolemoment,= electric dipole moment ,r= distance of point P from the center of dipole)<br>(\cos 60^{}^{\circ} = 1/2)

Options

  1. A18πε0pr2\dfrac{1}{8\pi\varepsilon_0}\dfrac{p}{r^2}
  2. B−18πε0pr2\dfrac{-1}{8\pi\varepsilon_0}\dfrac{p}{r^2}
  3. C−18πε03pr2\dfrac{-1}{8\pi\varepsilon_0}\dfrac{3p}{r^2}
  4. D18πε03pr2\dfrac{1}{8\pi\varepsilon_0}\dfrac{3p}{r^2}

Correct answer

B. −18πε0pr2\dfrac{-1}{8\pi\varepsilon_0}\dfrac{p}{r^2}

Step-by-step solution

The electric potential VV due to a dipole at a distance rr and angle θ\theta from the dipole axis is given by

V=14πε0pcos⁡θr2V = \dfrac{1}{4\pi\varepsilon_0} \dfrac{p \cos\theta}{r^2}

Given \theta = 120^{}^{\circ}, we have \cos 120^{}^{\circ} = -\cos 60^{}^{\circ} = -\dfrac{1}{2}

Substituting this value into the formula, we get

V=14πε0p(−12)r2V = \dfrac{1}{4\pi\varepsilon_0} \dfrac{p \left(-\dfrac{1}{2}\right)}{r^2}

V=−18πε0pr2V = \dfrac{-1}{8\pi\varepsilon_0} \dfrac{p}{r^2}

Answer: −18πε0pr2\dfrac{-1}{8\pi\varepsilon_0}\dfrac{p}{r^2}
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