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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 ' V ' at a radial distance x just outside a...

The electric potential ' VV ' at a radial distance xx just outside a non-conducting sphere is ρR22ε0x\dfrac{\rho R^2}{2 \varepsilon_0 x}. The electric intensity ' E ' at a radial distance xx is ( ρ\rho is uniform volume charge density, RR is the radius of the sphere and ε0\varepsilon_0 is the permittivity of free space)

Options

  1. AρR22ε0x\dfrac{\rho R^2}{2\varepsilon_0 x}
  2. BρR23ε0x2\dfrac{\rho R^2}{3\varepsilon_0 x^2}
  3. CρR22ε0x2\dfrac{\rho R^2}{2\varepsilon_0 x^2}
  4. DρR2ε0x2\dfrac{\rho R^2}{\varepsilon_0 x^2}

Correct answer

A. ρR22ε0x\dfrac{\rho R^2}{2\varepsilon_0 x}

Step-by-step solution

The relation between electric field intensity EE and electric potential VV in a radial field is given by E=−dVdxE = -\dfrac{dV}{dx}.

Given the electric potential V=ρR22ε0xV = \dfrac{\rho R^2}{2\varepsilon_0 x}.

Differentiating VV with respect to xx to find EE:

E=−ddx(ρR22ε0x)<br><br>E = -\dfrac{d}{dx} \left(\dfrac{\rho R^2}{2\varepsilon_0 x}\right)<br><br>E = -ρR22ε0(−1x2)<\dfrac{\rho R^2}{2\varepsilon_0} \left(-\dfrac{1}{x^2}\right)< br>
E=ρR22ε0x2E = \dfrac{\rho R²}{2\varepsilon_0 x²} Answer: ρR22ϵ0x\dfrac{\rho R²}{2\epsilon_0 x}
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