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BITSAT 2016
Exam
BITSAT
Year
2016
Subject
Physics
Chapter
Electromagnetic Induction

BITSAT 2016 · Physics · Electromagnetic Induction

An inductor of inductance L=400 mH and resistors of resistance R_ 1...

An inductor of inductance L=400mHL=400 \mathrm{mH} and resistors of resistance R1=2ΩR_{1}=2 \Omega and R2=2ΩR_{2}=2 \Omega are connected to a battery of emf 12V12 \mathrm{ V} as shown in the figure. The internal resistance of the battery is negligible. The switch SS is closed at t=0.t=0. The potential drop across LL as a function of time is An inductor of inductance L=400 mH and resistors of resistance R_ 1 =2 and R_ 2 =2 are connected to a battery of emf 12

Options

  1. A12te−3tV\frac{12}{t} e^{-3 t} \mathrm{ V}
  2. B6(1−e−t/0.2)V6\left(1-e^{-t / 0.2}\right) \mathrm{V}
  3. C12\mathrme−5tV12 \mathrme^{-5 t} \mathrm{ V}
  4. D6\mathrme−5tV6 \mathrme^{-5 t} \mathrm{ V}

Correct answer

C. 12\mathrme−5tV12 \mathrme^{-5 t} \mathrm{ V}

Step-by-step solution

Growth in current in LR2L R_{2} branch when switch is closed is given by i=ER2[1−e−R2t/L]⇒didt=ER2⋅R2Le−R2t/L=ELe−R2tL\begin{array}{l}i=\frac{E}{R_{2}}\left[1-e^{-R_{2} t / L}\right] \\ \Rightarrow \frac{d i}{d t}=\frac{E}{R_{2}} \cdot \frac{R_{2}}{L}e^{-R_{2} t / L}=\frac{E}{L}e^{-\frac{R_{2} t}{L}} \end{array}Hence, potential drop across $\mathbf{L}=\left(\frac{E}{L} e^{-R_{2} t / L}\right) L=E e^{-R_{2} t / L}=12 e^{-\frac{2 t}{400 \times 10^{-3}}}=12 \mathrme^{-5 t} \mathrm{~V}
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