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NEET PHYSICSMedium

Two charged spherical conductors of radii R1R_1 and R2R_2 are connected by a wire. The ratio of surface charge densities of spheres (σ1/σ2)(\sigma_1/\sigma_2) is:

A

\sqrt{\frac{R_1}{R_2}}

B

\frac{R_1^2}{R_2^2}

C

\frac{R_1}{R_2}

D

\frac{R_2}{R_1}

Step-by-Step Solution

  1. Common Potential: When two charged conductors are connected by a wire, charge flows between them until they reach the same electrostatic potential (VV). Thus, V1=V2V_1 = V_2.
  2. Formula for Potential: The potential of a charged sphere of radius RR and charge QQ is V=14πε0QRV = \frac{1}{4\pi\varepsilon_0} \frac{Q}{R}.
  3. Equating Potentials: Q1R1=Q2R2    Q1Q2=R1R2\frac{Q_1}{R_1} = \frac{Q_2}{R_2} \implies \frac{Q_1}{Q_2} = \frac{R_1}{R_2}.
  4. Surface Charge Density (σ\sigma): σ=ChargeArea=Q4πR2\sigma = \frac{\text{Charge}}{\text{Area}} = \frac{Q}{4\pi R^2}. Thus, Q=σ(4πR2)Q = \sigma(4\pi R^2).
  5. Substitute and Solve: σ1(4πR12)σ2(4πR22)=R1R2\frac{\sigma_1(4\pi R_1^2)}{\sigma_2(4\pi R_2^2)} = \frac{R_1}{R_2} σ1σ2R12R22=R1R2\frac{\sigma_1}{\sigma_2} \cdot \frac{R_1^2}{R_2^2} = \frac{R_1}{R_2} σ1σ2=R1R2R22R12=R2R1\frac{\sigma_1}{\sigma_2} = \frac{R_1}{R_2} \cdot \frac{R_2^2}{R_1^2} = \frac{R_2}{R_1}.
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