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JEE Main 202311 AprilMorning Shift
Exam
JEE Main
Year
2023
Date
11 April
Shift
Morning Shift
Subject
Physics
Chapter
Capacitance

JEE Main 2023 · 11 April · Morning Shift · Physics · Capacitance

A parallel plate capacitor of capacitance 2F is charged to a...

A parallel plate capacitor of capacitance 2F2F is charged to a potential VV. The energy stored in the capacitor is E1{E}_{1}. The capacitor is now connected to another uncharged identical capacitor in parallel combination. The energy stored in the combination is E2{E}_{2}. The ratio E2E1\dfrac{{E}_{2}}{{E}_{1}} isA parallel plate capacitor of capacitance 2F is charged to a potential V . The energy stored in the capacitor is E _ 1

Options

  1. A2:12: 1
  2. B2:32: 3
  3. C1:21: 2
  4. D1:41: 4

Correct answer

C. 1:21: 2

Step-by-step solution

The charge on the plates of the first capacitor when connected against the potential difference VV is given by

{Q=CV=2V\begin{cases}Q & = & CV \\ = & 2V\end{cases}

A parallel plate capacitor of capacitance 2F is charged to a potential V . The energy stored in the capacitor is E _ 1

When both the capacitors are connected, from the conservation of charge, it can be written that

{2V=2V′+2V′⇒V′=(12V)\begin{cases}2V & = & 2{V}^{'} + 2{V}^{'} \\ ⇒ & {V}^{'} = \left(\dfrac{1}{2}V\right)\end{cases}

where, V′V ' is the new potential difference across each capacitor.

The formula to calculate the energy stored in the first capacitor is given by

{E1=12×C×V2=12×2×V2=V2...(1)\begin{cases}{E}_{1} & = & \dfrac{1}{2} \times C \times {V}^{2} \\ = & \dfrac{1}{2} \times 2 \times {V}^{2} \\ = & {V}^{2} . . . \left(1\right)\end{cases}

For the second case, the energy stored in the combination of capacitor is given by

{E2=12nCV′2=12×2×V24×2=(V22)...(2)\begin{cases}{E}_{2} & = & \dfrac{1}{2}nCV{'}^{2} \\ = & \dfrac{1}{2} \times 2 \times \dfrac{{V}^{2}}{4} \times 2 \\ = & \left(\dfrac{{V}^{2}}{2}\right) . . . \left(2\right)\end{cases}

Divide equation (2) by equation (1) to obtain the required ratio of the stored energy.

{E2E1=V22V2=(12)\begin{cases}\dfrac{{E}_{2}}{{E}_{1}} & = & \dfrac{\dfrac{{V}^{2}}{2}}{{V}^{2}} \\ = & \left(\dfrac{1}{2}\right)\end{cases}

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