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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 initially provided with a...

A capacitor having capacitance CC is initially provided with a charge QQ. At t=0t = 0, it is linked to an ideal battery of emf E\mathcal{E} via a resistance RR. Determine the charge on the capacitor at time tt.

Options

  1. A(CE+Q)(C\mathcal{E} + Q)\left(1 - e^{-\dfrac{t}{CR}}\right)
  2. BCEe−tCR+QC\mathcal{E} e^{-\dfrac{t}{CR}} + Q\left(1 - e^{-\dfrac{t}{CR}}\right)
  3. CCE(1−e−tCR)−Qe−tCRC\mathcal{E}\left(1 - e^{-\dfrac{t}{CR}}\right) - Q e^{-\dfrac{t}{CR}}
  4. DCE(1−e−tCR)+Qe−tCRC\mathcal{E}\left(1 - e^{-\dfrac{t}{CR}}\right) + Q e^{-\dfrac{t}{CR}}

Correct answer

D. CE(1−e−tCR)+Qe−tCRC\mathcal{E}\left(1 - e^{-\dfrac{t}{CR}}\right) + Q e^{-\dfrac{t}{CR}}

Step-by-step solution

Applying Kirchhoff's loop rule for the circuit at time tt:

E−iR−qC=0\mathcal{E} - iR - \dfrac{q}{C} = 0

Substituting i=dqdti = \dfrac{dq}{dt}:

Rdqdt=E−qC=CE−qCR \dfrac{dq}{dt} = \mathcal{E} - \dfrac{q}{C} = \dfrac{C\mathcal{E} - q}{C}

Rearranging and integrating with the initial condition q(0)=Qq(0) = Q:

∫QqdqCE−q=∫0tdtRC\int_Q^{q} \dfrac{dq}{C\mathcal{E} - q} = \int_{0}^{t} \dfrac{dt}{RC}

[−ln⁡(CE−q)]Qq=tRC[-\ln(C\mathcal{E} - q)]_Q^{q} = \dfrac{t}{RC}

ln⁡(CE−qCE−Q)=−tRC\ln\left(\dfrac{C\mathcal{E} - q}{C\mathcal{E} - Q}\right) = -\dfrac{t}{RC}

CE−q=(CE−Q)e−tRCC\mathcal{E} - q = (C\mathcal{E} - Q) e^{-\dfrac{t}{RC}}

q=CE(1−e−tRC)+Qe−tRCq = C\mathcal{E}\left(1 - e^{-\dfrac{t}{RC}}\right) + Q e^{-\dfrac{t}{RC}}
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