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A capacitor of capacitance C0 is charged...

A capacitor of capacitance `C_0` is charged to potential `V_0`. Now it is connected to another uncharged capacitor of capacitance `C_0/2`. Calculate the heat loss in this process.

A

`1/2 C_0 V_0^2`

B

`1/3 C_0 V_0^2`

C

`1/6 C_0 V_0^2`

D

`1/8 C_0 V_0^2`

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To solve the problem of calculating the heat loss when a charged capacitor is connected to an uncharged capacitor, we can follow these steps: ### Step-by-Step Solution: 1. **Identify Initial Conditions**: - A capacitor of capacitance \( C_0 \) is charged to a potential \( V_0 \). - The charge on this capacitor is given by: \[ Q_0 = C_0 V_0 \] 2. **Connect to Another Capacitor**: - The charged capacitor \( C_0 \) is connected to an uncharged capacitor of capacitance \( \frac{C_0}{2} \). - After connection, the total charge \( Q_0 \) will redistribute between the two capacitors. 3. **Determine Final Voltage**: - Let the final voltage across both capacitors after connection be \( V_{AB} \). - The charge on the first capacitor (charged one) will be: \[ Q_1 = C_0 V_{AB} \] - The charge on the second capacitor (uncharged one) will be: \[ Q_2 = \frac{C_0}{2} V_{AB} \] 4. **Conservation of Charge**: - According to the conservation of charge: \[ Q_1 + Q_2 = Q_0 \] - Substituting the expressions for \( Q_1 \) and \( Q_2 \): \[ C_0 V_{AB} + \frac{C_0}{2} V_{AB} = C_0 V_0 \] - Factor out \( V_{AB} \): \[ V_{AB} \left( C_0 + \frac{C_0}{2} \right) = C_0 V_0 \] - Simplifying gives: \[ V_{AB} \left( \frac{3C_0}{2} \right) = C_0 V_0 \] - Thus, the final voltage \( V_{AB} \) is: \[ V_{AB} = \frac{2V_0}{3} \] 5. **Calculate Initial and Final Potential Energy**: - The initial potential energy \( U_i \) of the charged capacitor is: \[ U_i = \frac{1}{2} C_0 V_0^2 \] - The final potential energy \( U_f \) of the system (both capacitors) is: \[ U_f = \frac{1}{2} C_0 V_{AB}^2 + \frac{1}{2} \left( \frac{C_0}{2} \right) V_{AB}^2 \] - Substituting \( V_{AB} = \frac{2V_0}{3} \): \[ U_f = \frac{1}{2} C_0 \left( \frac{2V_0}{3} \right)^2 + \frac{1}{2} \left( \frac{C_0}{2} \right) \left( \frac{2V_0}{3} \right)^2 \] - Calculating each term: \[ U_f = \frac{1}{2} C_0 \cdot \frac{4V_0^2}{9} + \frac{1}{4} C_0 \cdot \frac{4V_0^2}{9} = \frac{2C_0 V_0^2}{9} + \frac{C_0 V_0^2}{9} = \frac{3C_0 V_0^2}{9} = \frac{C_0 V_0^2}{3} \] 6. **Calculate Heat Loss**: - The heat loss \( Q \) during this process is the change in potential energy: \[ Q = U_i - U_f = \frac{1}{2} C_0 V_0^2 - \frac{C_0 V_0^2}{3} \] - Finding a common denominator (6): \[ Q = \frac{3C_0 V_0^2}{6} - \frac{2C_0 V_0^2}{6} = \frac{C_0 V_0^2}{6} \] ### Final Answer: The heat loss in this process is: \[ \boxed{\frac{C_0 V_0^2}{6}} \]
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