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Concepts Of Physics MCQ Edition [Volume 2]
Exam
Concepts Of Physics MCQ Edition [Volume 2]
Subject
Physics
Chapter
Electric Current in Conductors

Concepts Of Physics MCQ Edition [Volume 2] · Physics · Electric Current in Conductors

A capacitor having capacitance C is given an initial charge Q . At...

A capacitor having capacitance CC is given an initial charge QQ. At time t=0t = 0, it is connected across an uncharged capacitor of the same capacitance via a resistance RR. Determine the charge accumulated on the second capacitor as a function of time.

Options

  1. AQ(1−e−t/RC)Q(1 - e^{-t/RC})
  2. BQ2(1−e−2t/RC)\dfrac{Q}{2}(1 - e^{-2t/RC})
  3. CQ(1−e−2t/RC)Q(1 - e^{-2t/RC})
  4. DQ2(1−e−t/RC)\dfrac{Q}{2}(1 - e^{-t/RC})

Correct answer

B. Q2(1−e−2t/RC)\dfrac{Q}{2}(1 - e^{-2t/RC})

Step-by-step solution

Let q1q_1 and q2q_2 be the charges on the first and second capacitors at time tt.

By conservation of charge, q1+q2=Qq_1 + q_2 = Q.

Applying Kirchhoff's voltage law in the circuit:

q1C−iR−q2C=0\dfrac{q_1}{C} - iR - \dfrac{q_2}{C} = 0

Since i=dq2dti = \dfrac{dq_2}{dt} and q1=Q−q2q_1 = Q - q_2, we have:

Q−q2C−q2C=Rdq2dt\dfrac{Q - q_2}{C} - \dfrac{q_2}{C} = R \dfrac{dq_2}{dt}

Q−2q2C=Rdq2dt\dfrac{Q - 2q_2}{C} = R \dfrac{dq_2}{dt}

dq2Q−2q2=dtRC\dfrac{dq_2}{Q - 2q_2} = \dfrac{dt}{RC}

Integrating both sides with limits q2=0q_2 = 0 at t=0t = 0 to q2q_2 at time tt:

∫0q2dq2Q−2q2=∫0tdtRC\int_{0}^{q_2} \dfrac{dq_2}{Q - 2q_2} = \int_{0}^{t} \dfrac{dt}{RC}

−12ln⁡(Q−2q2Q)=tRC-\dfrac{1}{2} \ln \left( \dfrac{Q - 2q_2}{Q} \right) = \dfrac{t}{RC}

ln⁡(Q−2q2Q)=−2tRC\ln \left( \dfrac{Q - 2q_2}{Q} \right) = -\dfrac{2t}{RC}

Q−2q2=Qe−2t/RCQ - 2q_2 = Q e^{-2t/RC}

q2=Q2(1−e−2t/RC)q_2 = \dfrac{Q}{2}(1 - e^{-2t/RC})
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