Home
Class 12
PHYSICS
A series combination of n(1) capacitors,...

A series combination of `n_(1)` capacitors, each of value `C_(1)`, is charged by a source of potential difference `4 V`. When another parallel combination of `n_(2)` capacitors, each of value `C_(2)`, is charged by a source of potential difference `V`, it has same (total) energy stored in it, as the first combination has. the value of `C_(2)`, in terms of `C_(1)`, is then

A

`(2C_(1))/(n_(1)n_(2))`

B

`16(n_(2))/(n_(1))C_(1)`

C

`2(n_(2))/(n_(1))C_(1)`

D

`(16C_(1))/(n_(1)n_(2))`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the value of \( C_2 \) in terms of \( C_1 \) given that the total energy stored in a series combination of capacitors is equal to the total energy stored in a parallel combination of capacitors. ### Step-by-step Solution: 1. **Understand the Series Combination of Capacitors:** For \( n_1 \) capacitors in series, each with capacitance \( C_1 \), the equivalent capacitance \( C_s \) is given by: \[ C_s = \frac{C_1}{n_1} \] 2. **Calculate the Energy Stored in the Series Combination:** The energy \( U_s \) stored in a capacitor is given by the formula: \[ U = \frac{1}{2} C V^2 \] For the series combination charged by a potential difference of \( 4V \): \[ U_s = \frac{1}{2} C_s (4V)^2 = \frac{1}{2} \left(\frac{C_1}{n_1}\right) (4V)^2 \] Simplifying this gives: \[ U_s = \frac{1}{2} \left(\frac{C_1}{n_1}\right) (16V^2) = \frac{8C_1 V^2}{n_1} \] 3. **Understand the Parallel Combination of Capacitors:** For \( n_2 \) capacitors in parallel, each with capacitance \( C_2 \), the equivalent capacitance \( C_p \) is given by: \[ C_p = n_2 C_2 \] 4. **Calculate the Energy Stored in the Parallel Combination:** The energy \( U_p \) stored in the parallel combination charged by a potential difference \( V \): \[ U_p = \frac{1}{2} C_p V^2 = \frac{1}{2} (n_2 C_2) V^2 \] This simplifies to: \[ U_p = \frac{1}{2} n_2 C_2 V^2 \] 5. **Set the Energies Equal:** Since the total energy stored in both combinations is the same, we can set \( U_s = U_p \): \[ \frac{8C_1 V^2}{n_1} = \frac{1}{2} n_2 C_2 V^2 \] 6. **Simplify the Equation:** We can cancel \( V^2 \) from both sides (assuming \( V \neq 0 \)): \[ \frac{8C_1}{n_1} = \frac{1}{2} n_2 C_2 \] 7. **Rearranging to Find \( C_2 \):** Multiply both sides by \( 2 \): \[ \frac{16C_1}{n_1} = n_2 C_2 \] Now, solve for \( C_2 \): \[ C_2 = \frac{16C_1}{n_1 n_2} \] ### Final Answer: \[ C_2 = \frac{16C_1}{n_1 n_2} \]
Promotional Banner

Similar Questions

Explore conceptually related problems

Find the energy stored in a capacitor of capacitance 100muF when it is charged to a potential difference of 20 V.

A capacitor is charged through a potential difference of 200 V, when 0.1C charge is stored in it. The amount of energy released by it, when it is discharged is

A capacitor when charged by a potential difference of 200 Volts, stores a charge of 0.1C. By discharging energy liberated by the capacitor is-

A capacitor or capacitance C_(1) is charge to a potential V and then connected in parallel to an uncharged capacitor of capacitance C_(2) . The fianl potential difference across each capacitor will be

A capacitor of capacitance C, charged to a potential difference V, is discharged through a series combination of two resistors R_(1) and R_(2) . Find the heat generated in resistor R_(1) during discharging.

A capacitor of capacitance C_(1) is charged to a potential difference V and then connected with an uncharged capacitor of capacitance C_(2) a resistance R. The switch is closed at t = 0. Choose the correct option(s):

A capacitor of capacitance C_(1) is charged to a potential V_(1) while another capacitor of capacitance C_(2) is charged to a potential difference V_(2) . The capacitors are now disconnected from their respective charging batteries and connected in parallel to each other . (a) Find the total energy stored in the two capacitors before they are connected. (b) Find the total energy stored in the parallel combination of the two capacitors. (c ) Explain the reason for the difference of energy in parallel combination in comparison to the total energy before they are connected.

A capacitor of capacitance C is charged to a potential difference V_(0) . The charged battery is disconnected and the capacitor is connected to a capacitor of unknown capacitance C_(x) . The potential difference across the combination is V. The value of C_(x) should be

A parallel plate capacitor of capacitance C is connected to a battery and is charged to a potential difference V. Another capacitor of capacitance 2C is ismilarly charged to a potential difference 2V. The charging battery is now disconnected and the capacitors are connected in parallel to each other in such a way that the poistive terminal of one is connected to the negative terminal of the other. The final energy of the configuration is

n identical capacitors are connected in parallel to a potential difference V . These capacitors are then reconnected in series, their charges being left undisturbed. The potential difference obtained is