JEE Challenger
More from Electrostatic Potential and Capacitance

Magnitude of Final Capacitor Charge when Switch is Shifted to Position Q

Comprehension Passage

In the circuit diagram shown below, switch SS is maintained at position PP for a sufficiently long time such that the charge stored on the capacitor is q1 μCq_1\ \mu\text{C}. Switch SS is then flipped to position QQ. After a long time, the charge on the capacitor becomes q2 μCq_2\ \mu\text{C}.

Determine the magnitude of q2q_2.

Question Diagram 1
Official Numerical Answer0.66 to 0.67

Step-by-Step Solution

To find the magnitude of the final charge q2q_2 on the capacitor, we analyze the circuit in its steady state after the switch SS is moved to position QQ.

1. Circuit Description and Reference Potentials

Let the bottom wire of the circuit be chosen as the reference node with zero potential: Vbottom=0 VV_{\text{bottom}} = 0\text{ V}

  • Switch at position QQ: Position QQ is directly connected to the bottom reference wire, so the potential at terminal QQ is: VQ=0 VV_Q = 0\text{ V}

  • Far-right branch: The positive terminal of the 2 V2\text{ V} battery is at a potential of +2 V+2\text{ V} relative to the bottom wire.

  • Capacitor branch: A 1 μF1\ \mu\text{F} capacitor is connected between the central node (let's call it node AA) and the bottom reference wire (0 V0\text{ V}).


2. Steady-State Analysis for Switch at Position QQ

In a DC circuit, after a sufficiently long time (steady state), the capacitor behaves as an open circuit (i.e., no current flows through the capacitor branch).

Therefore, current flows only through the outer loop containing the 1 Ω1\ \Omega resistor, node AA, the 2 Ω2\ \Omega resistor, and the 2 V2\text{ V} battery.

Applying Kirchhoff's Current Law (KCL) at node AA: VA−VQ1 Ω+VA−2 V2 Ω=0\frac{V_A - V_Q}{1\ \Omega} + \frac{V_A - 2\text{ V}}{2\ \Omega} = 0

Substitute VQ=0 VV_Q = 0\text{ V}: VA−01+VA−22=0\frac{V_A - 0}{1} + \frac{V_A - 2}{2} = 0

VA+0.5VA−1=0V_A + 0.5 V_A - 1 = 0

1.5VA=1  ⟹  VA=23 V1.5 V_A = 1 \implies V_A = \frac{2}{3}\text{ V}


3. Calculation of Charge q2q_2

The charge stored on the 1 μF1\ \mu\text{F} capacitor in this steady state is given by: q2=C⋅VA=(1 μF)×(23 V)=23 μC≈0.67 μCq_2 = C \cdot V_A = (1\ \mu\text{F}) \times \left(\frac{2}{3}\text{ V}\right) = \frac{2}{3}\ \mu\text{C} \approx 0.67\ \mu\text{C}

Thus, the magnitude of q2q_2 is 0.670.67 (or 23\frac{2}{3}).