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NEET PHYSICSEasy

The variation of electrostatic potential with radial distance rr from the centre of a positively charged metallic thin shell of radius RR is given by the graph:

A

Option 1

B

Option 2

C

Option 3

D

Option 4

Step-by-Step Solution

  1. Inside the Shell (r<Rr < R): According to the property of electrostatic shielding (mentioned in Class 11 Physics, Points to Ponder [1]), the electric field EE inside a charged hollow conductor is zero. Since the electric field is the gradient of the potential (E=dV/drE = -dV/dr), a zero field implies that the potential VV is constant throughout the interior. Its value is equal to the potential at the surface: V=14πε0QRV = \frac{1}{4\pi\varepsilon_0}\frac{Q}{R}.
  2. Outside the Shell (rRr \geq R): For points outside, the shell behaves as if the entire charge QQ were concentrated at its center (analogous to the gravitational case for a spherical shell discussed in Class 11 Physics [2]). Thus, the potential decreases inversely with distance: V=14πε0QrV = \frac{1}{4\pi\varepsilon_0}\frac{Q}{r}.
  3. Graph Characteristics: The correct graph starts at a positive constant value for rr from 00 to RR, and then decreases as a hyperbola (1/r1/r) for r>Rr > R. This corresponds to the standard behavior described in Option 2.
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