Step 1: Understanding Potential on a Conducting Sphere The potential \( V \) of a charged conducting sphere of radius \( R \) carrying charge \( Q \) is given by: \[ V = \frac{1}{4\pi \varepsilon_0} \frac{Q}{R} \] When two conductors are connected by a wire, charge flows until their potentials become equal.
Step 2: Finding Initial Potentials of Spheres A and B For sphere A: \[ V_A = \frac{Q_A}{R_A} = \frac{80}{4} = 20 \text{ V} \] For sphere B: \[ V_B = \frac{Q_B}{R_B} = \frac{40}{6} = 6.67 \text{ V} \] Since \( V_A>V_B \), charge will flow from sphere A to sphere B until their potentials equalize.
Step 3: Finding Common Potential After connection, the total charge is conserved, and the final common potential \( V_f \) is given by: \[ V_f = \frac{Q_A + Q_B}{R_A + R_B} \] \[ V_f = \frac{80 + 40}{4 + 6} = \frac{120}{10} = 12 \text{ V} \]
Step 4: Charge Redistribution Using \( Q = V_f R \), the final charges on A and B will be: \[ Q_A' = V_f \times R_A = 12 \times 4 = 48 \text{ µC} \] \[ Q_B' = V_f \times R_B = 12 \times 6 = 72 \text{ µC} \] The charge transfer is: \[ \Delta Q = Q_B' - Q_B = 72 - 40 = 32 \text{ µC} \] Since charge increases on B, the charge flows from B to A.
Final Answer: \( 32 \) µC flows from B to A.
Match List - I with List - II:
List - I:
(A) Electric field inside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(B) Electric field at distance \( r > 0 \) from a uniformly charged infinite plane sheet with surface charge density \( \sigma \).
(C) Electric field outside (distance \( r > 0 \) from center) of a uniformly charged spherical shell with surface charge density \( \sigma \), and radius \( R \).
(D) Electric field between two oppositely charged infinite plane parallel sheets with uniform surface charge density \( \sigma \).
List - II:
(I) \( \frac{\sigma}{\epsilon_0} \)
(II) \( \frac{\sigma}{2\epsilon_0} \)
(III) 0
(IV) \( \frac{\sigma}{\epsilon_0 r^2} \) Choose the correct answer from the options given below: