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Two concentric hollow conducting spheres...

Two concentric hollow conducting spheres of radius a and b `(b gt a)` contains charges `Q_(a)` and `Q_(b)` respectively. If they are connected by a conducting wire then find out following
(i) Final charges on inner and outer spheres.
(ii) Heat produced during the process.

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To solve the problem of two concentric hollow conducting spheres with charges \( Q_a \) and \( Q_b \), we will follow these steps: ### Step 1: Understand the System We have two concentric hollow conducting spheres: - Inner sphere with radius \( a \) and charge \( Q_a \) - Outer sphere with radius \( b \) and charge \( Q_b \) When connected by a conducting wire, the charges will redistribute until the potential on both spheres is equal. ### Step 2: Use the Concept of Electric Potential For a conducting sphere, the electric potential \( V \) at the surface is given by: \[ V = \frac{kQ}{R} \] where \( k \) is the Coulomb's constant, \( Q \) is the charge, and \( R \) is the radius of the sphere. - For the inner sphere (radius \( a \)): \[ V_a = \frac{kQ_a}{a} \] - For the outer sphere (radius \( b \)): \[ V_b = \frac{kQ_b}{b} \] ### Step 3: Set the Potentials Equal Since the spheres are connected by a wire, the potentials must be equal: \[ \frac{kQ_a'}{a} = \frac{kQ_b'}{b} \] where \( Q_a' \) and \( Q_b' \) are the final charges on the inner and outer spheres, respectively. ### Step 4: Conservation of Charge The total charge before and after connecting the spheres must be conserved: \[ Q_a + Q_b = Q_a' + Q_b' \] ### Step 5: Solve the Equations From the potential equality, we can express \( Q_b' \) in terms of \( Q_a' \): \[ Q_b' = \frac{b}{a} Q_a' \] Substituting this into the conservation of charge equation: \[ Q_a + Q_b = Q_a' + \frac{b}{a} Q_a' \] \[ Q_a + Q_b = Q_a' \left(1 + \frac{b}{a}\right) \] \[ Q_a' = \frac{Q_a + Q_b}{1 + \frac{b}{a}} = \frac{(Q_a + Q_b) a}{a + b} \] Now substituting \( Q_a' \) back to find \( Q_b' \): \[ Q_b' = \frac{b}{a} Q_a' = \frac{b}{a} \cdot \frac{(Q_a + Q_b) a}{a + b} = \frac{b(Q_a + Q_b)}{a + b} \] ### Step 6: Final Charges Thus, the final charges on the inner and outer spheres are: \[ Q_a' = \frac{(Q_a + Q_b) a}{a + b} \] \[ Q_b' = \frac{b(Q_a + Q_b)}{a + b} \] ### Step 7: Calculate Heat Produced The heat produced during the process can be calculated by finding the difference in potential energy before and after the connection. Initial potential energy \( U_i \): \[ U_i = \frac{k Q_a^2}{2a} + \frac{k Q_b^2}{2b} \] Final potential energy \( U_f \): \[ U_f = \frac{k (Q_a')^2}{2a} + \frac{k (Q_b')^2}{2b} \] The heat produced \( Q \) is given by: \[ Q = U_i - U_f \] ### Step 8: Substitute and Simplify Substituting the expressions for \( U_i \) and \( U_f \) and simplifying will yield the total heat produced. ### Final Answers (i) Final charges: \[ Q_a' = \frac{(Q_a + Q_b) a}{a + b} \] \[ Q_b' = \frac{b(Q_a + Q_b)}{a + b} \] (ii) Heat produced: \[ Q = U_i - U_f \]
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