This problem is a beautiful masterclass in understanding the transient and steady-state behaviors of RC circuits. It tests your ability to apply the fundamental rules of capacitors at three distinct moments in time: exactly when a switch is closed (t=0), after a long time (t→∞), and the exact instant a new switch is introduced to a steady-state system.
Let's break down the circuit and evaluate each option systematically.
Phase 1
The Initial State (t=0)
Let's test Option (C) first. At time t=0, the switch S1 is closed while S2 remains open.
The Golden Rule: The moment a circuit is completed, an uncharged capacitor acts as a perfect short circuit (a simple wire) because there is no accumulated charge to oppose the flow of current.
Since S2 is open, the middle branch is completely disconnected. The circuit simplifies to a single, large outer loop containing the 5V battery and three resistors in series. The total equivalent resistance is simply the sum of these resistors:
Req=70 Ω+30 Ω+100 Ω=200 Ω
Using Ohm's law, the instantaneous current flowing through this closed circuit is:
i=ReqVnet=200 Ω5V=0.025A=25mA
This perfectly matches Option (C), making it a correct statement.
Phase 2
The Steady State (t→∞)
Now, let's evaluate Options (B) and (D). If switch S1 is kept closed for a long time, the circuit reaches a steady state.
The Golden Rule: In a DC circuit, a fully charged capacitor acts as an open circuit, completely blocking the flow of direct current.
With the current dropping to zero, there is no voltage drop across any of the resistors. However, the capacitors have stored charge. Because they are all part of the same single loop, the capacitors C1, C4, and C3 are effectively in series. We can find their equivalent capacitance:
Ceq1=101+801+801=8010
The total charge pumped by the 5V battery is:
Since they are in series, this exact same charge of 40 μC resides on each capacitor. We can now find the voltage across C1:
VC1=C1Q=10 μF40 μC=4V
This confirms that Option (D) is correct.
What about Option (B)? It asks for the voltage difference between points P and Q. Let's assume point Q (on the bottom wire) is at 0V. Since there is no current, there is no voltage drop across the 70 Ω resistor. The potential at point P is entirely determined by the voltage across C1, which we just calculated as 4V. Therefore, VP−VQ=4V, not 10V. Option (B) is incorrect.
Phase 3
The Transient State (Closing S2)
Finally, let's tackle Option (A). After reaching the steady state, switch S2 is suddenly closed.
The Golden Rule: The voltage across a capacitor cannot change instantaneously. At the exact moment a switch is closed (t=0+), capacitors maintain their stored voltage and act mathematically like ideal batteries.
Let's draw the equivalent circuit for this specific instant:
- Left Branch: C1 acts as a 4V battery in series with the 70 Ω resistor.
- Middle Branch: The uncharged C2 acts as a short circuit, leaving the 10V battery in series with the 30 Ω resistor.
- Right Branch: C4 and C3 both act as 0.5V batteries. Combining these with the 5V battery yields an equivalent 4V battery in series with a total resistance of 130 Ω (30 Ω+100 Ω).
Notice something beautiful here! Both the left and right branches have an equivalent voltage of 4V relative to ground. We can combine them into a single parallel branch with a 4V source and an equivalent resistance:
Req=70+13070×130=2009100=45.5 Ω
Now, we have a simple loop where the 10V battery in the middle branch opposes the combined 4V battery. The instantaneous current through the middle branch is:
i=30 Ω+45.5 Ω10V−4V=75.56≈0.079A
This is far from the 0.2A claimed in Option (A), making it incorrect.
By mastering these three phases, you can confidently dismantle any complex RC circuit problem!