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Question: In the given circuit C₁ = C, C₂ = 2C, V₁ = V₂ = V & R₁ = R₂ = R₃ = R and all switches-are closed at ...

In the given circuit C₁ = C, C₂ = 2C, V₁ = V₂ = V & R₁ = R₂ = R₃ = R and all switches-are closed at t = 0 then choose the incorrect statement at time t = RC (initially all capacitors are uncharged)

A

Current through V₁ is less than V2Re[e1]\frac{V}{2Re}[e-1]

B

Power delivered by V₂ is less than V23eR\frac{V^2}{3eR}

C

Current through V₁ is greater than V2Re[e1]\frac{V}{2Re}[e-1]

Answer

Incorrect statements are A and B.

Explanation

Solution

We will show that if we view the circuit as a single‐loop network so that the two sources “assist” each other (i.e. their EMFs add up to 2V), then the three resistors R₁, R₂ and R₃ (all equal to R) lie in series and the two capacitors (of capacitances C and 2C in series) have an equivalent capacitance

Ceq=C2CC+2C=2C3C_{eq} = \frac{C \cdot 2C}{C+2C} = \frac{2C}{3}.

Thus the overall time‐constant is

τ=(R1+R2+R3)Ceq=(3R)2C3=2RC\tau = (R₁ + R₂ + R₃) \cdot C_{eq} = (3R) \cdot \frac{2C}{3} = 2RC.

For a standard RC–circuit the current (if the net emf is 2V) is I(t)=2V3RetτI(t) = \frac{2V}{3R} \cdot e^{\frac{-t}{\tau}}.

At t = RC we have I(RC)=2V3ReRC2RC=2V3Re12I(RC) = \frac{2V}{3R} \cdot e^{\frac{-RC}{2RC}} = \frac{2V}{3R} \cdot e^{\frac{-1}{2}}.

Numerically, since e120.6065e^{\frac{-1}{2}} \approx 0.6065, I(RC)2V3R0.60650.4043VRI(RC) \approx \frac{2V}{3R} \cdot 0.6065 \approx 0.4043 \cdot \frac{V}{R}.

Now notice that the “benchmark” given in options A and C is

V2eR(e1)\frac{V}{2eR} \cdot (e - 1).

Since e ≈ 2.718, e – 1 ≈ 1.718 so that V2eR(e1)V5.436R1.7180.316VR\frac{V}{2eR} \cdot (e - 1) \approx \frac{V}{5.436R} \cdot 1.718 \approx 0.316 \cdot \frac{V}{R}.

Thus we have

I(RC)0.4043VR>0.316VRI(RC) \approx 0.4043 \frac{V}{R} > 0.316 \frac{V}{R}.

In other words, the current coming from V₁ is greater than the given benchmark value. Therefore:

  • Statement A (“Current through V₁ is less than …”) is false.
  • Statement C (“Current through V₁ is greater than …”) is correct.

Next, the power supplied by source V₂ (which—since the circuit is in series—has the same current I flowing through it) is

P2=VI(RC)V(0.4043VR)=0.4043V2RP₂ = V \cdot I(RC) \approx V \cdot (0.4043 \cdot \frac{V}{R}) = 0.4043 \cdot \frac{V^2}{R}.

But the option B claims that P2<V23eRP₂ < \frac{V^2}{3eR}.

Since 3e ≈ 8.154, we have V23eR0.1226V2R\frac{V^2}{3eR} \approx 0.1226 \cdot \frac{V^2}{R}. Clearly 0.4043V2R0.4043 \cdot \frac{V^2}{R} is not less than 0.1226V2R0.1226 \cdot \frac{V^2}{R}. Thus statement B is also false.

So, the incorrect statements (the “wrong” ones) are A and B.

Summary of Core Steps:

  1. The loop has three resistors (3R) and the series combination of C and 2C gives Ceq=2C3C_{eq} = \frac{2C}{3} so that τ = 2RC.
  2. With net emf 2V, the transient current is I(t)=2V3Ret2RCI(t) = \frac{2V}{3R} \cdot e^{\frac{-t}{2RC}}. At t = RC, I0.4043VRI \approx 0.4043 \cdot \frac{V}{R}.
  3. The given benchmark current is V2eR(e1)0.316VR\frac{V}{2eR}(e – 1) \approx 0.316 \cdot \frac{V}{R}. Thus statement A is false and C true.
  4. Also, power from V₂ is VI0.4043V2RV \cdot I \approx 0.4043 \cdot \frac{V^2}{R} which is not less than V23eR0.1226V2R\frac{V^2}{3eR} \approx 0.1226 \frac{V^2}{R}. So B is false.