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Question: In figure an arrangement of three identical capcitors is shown alongwith a switch S and a battery B....

In figure an arrangement of three identical capcitors is shown alongwith a switch S and a battery B. If the switch S is closed, then the ratio of the energy of the capacitors system in the final steady state to the initial state is :-

A

2:1

B

4:3

C

3:2

D

3:4

Answer

4:3

Explanation

Solution

To solve this problem, we need to calculate the total energy stored in the capacitor system in two different states:

  1. Initial state: When the switch S is open.
  2. Final steady state: When the switch S is closed.

Let the capacitance of each identical capacitor be CC, and the voltage of the battery be VV. The energy stored in a capacitor system is given by the formula U=12CeqV2U = \frac{1}{2} C_{eq} V^2, where CeqC_{eq} is the equivalent capacitance of the system.

1. Initial State (Switch S is open)

When the switch S is open, the capacitor connected in the branch with the switch (let's call it C2C_2) is disconnected from the circuit. The circuit effectively consists of the other two capacitors (C1C_1 and C3C_3) connected in series across the battery.

Since the path with C2C_2 is open, only C1C_1 and C3C_3 are active in the circuit. They are connected in series. The equivalent capacitance for two capacitors in series is given by: Ceq,initial=C1×C3C1+C3=C×CC+C=C22C=C2C_{eq, initial} = \frac{C_1 \times C_3}{C_1 + C_3} = \frac{C \times C}{C + C} = \frac{C^2}{2C} = \frac{C}{2}

The energy stored in the initial state is: Uinitial=12Ceq,initialV2=12(C2)V2=14CV2U_{initial} = \frac{1}{2} C_{eq, initial} V^2 = \frac{1}{2} \left(\frac{C}{2}\right) V^2 = \frac{1}{4} C V^2

2. Final Steady State (Switch S is closed)

When the switch S is closed, all three capacitors are part of the circuit.

This configuration means that C2C_2 and C3C_3 are connected in parallel, and this parallel combination is then connected in series with C1C_1.

First, calculate the equivalent capacitance of C2C_2 and C3C_3 in parallel: Cparallel=C2+C3=C+C=2CC_{parallel} = C_2 + C_3 = C + C = 2C

Now, this CparallelC_{parallel} is in series with C1C_1. The total equivalent capacitance of the system in the final state is: Ceq,final=C1×CparallelC1+Cparallel=C×(2C)C+2C=2C23C=2C3C_{eq, final} = \frac{C_1 \times C_{parallel}}{C_1 + C_{parallel}} = \frac{C \times (2C)}{C + 2C} = \frac{2C^2}{3C} = \frac{2C}{3}

The energy stored in the final steady state is: Ufinal=12Ceq,finalV2=12(2C3)V2=13CV2U_{final} = \frac{1}{2} C_{eq, final} V^2 = \frac{1}{2} \left(\frac{2C}{3}\right) V^2 = \frac{1}{3} C V^2

3. Ratio of Energies

Finally, we need to find the ratio of the energy in the final steady state to the initial state (Ufinal:UinitialU_{final} : U_{initial}). Ratio = UfinalUinitial=13CV214CV2\frac{U_{final}}{U_{initial}} = \frac{\frac{1}{3} C V^2}{\frac{1}{4} C V^2}

Cancel out the common terms (CV2C V^2): Ratio = 1/31/4=13×41=43\frac{1/3}{1/4} = \frac{1}{3} \times \frac{4}{1} = \frac{4}{3}

So, the ratio of the energy of the capacitors system in the final steady state to the initial state is 4:3.