Sign in
12thPass logo
New chatPYQ LibraryDoubtsRank report
Sign in to see Recents

Your guest activity stays on this device

Sign in to save progress →
Sign in

Capacitor question

2021 · 27 Jul · Shift 2 · Q53
Guest · filters and generic practice availableBrowsing as a guest · PYQ filters and generic practice are available. Sign in only for personalised features and saved progress.
  1. PYQ Library
  2. /JEE Main
  3. /Physics
  4. /Capacitor
  5. /2021 · 27 Jul · Shift 2 · Q53

Capacitor question

2021 · 27 Jul · Shift 2 · Q53

JEE MainPhysicsCapacitorMCQ+4 / −1
A simple pendulum of mass 'm', length 'l' and charge '+ q' suspended in the electric field produced by two conducting parallel plates as shown. The value of deflection of pendulum in equilibrium position will be JEE Main 2021 (Online) 27th July Evening Shift Physics - Capacitor Question 83 English
  1. A
    tan⁡−1[qmg×C1(V2−V1)(C1+C2)(d−t)]{\tan ^{ - 1}}\left[ {{q \over {mg}} \times {{{C_1}({V_2} - {V_1})} \over {({C_1} + {C_2})(d - t)}}} \right]tan−1[mgq​×(C1​+C2​)(d−t)C1​(V2​−V1​)​]
  2. B
    tan⁡−1[qmg×C2(V2−V1)(C1+C2)(d−t)]{\tan ^{ - 1}}\left[ {{q \over {mg}} \times {{{C_2}({V_2} - {V_1})} \over {({C_1} + {C_2})(d - t)}}} \right]tan−1[mgq​×(C1​+C2​)(d−t)C2​(V2​−V1​)​]
  3. C
    tan⁡−1[qmg×C2(V1+V2)(C1+C2)(d−t)]{\tan ^{ - 1}}\left[ {{q \over {mg}} \times {{{C_2}({V_1} + {V_2})} \over {({C_1} + {C_2})(d - t)}}} \right]tan−1[mgq​×(C1​+C2​)(d−t)C2​(V1​+V2​)​]
  4. D
    tan⁡−1[qmg×C1(V1+V2)(C1+C2)(d−t)]{\tan ^{ - 1}}\left[ {{q \over {mg}} \times {{{C_1}({V_1} + {V_2})} \over {({C_1} + {C_2})(d - t)}}} \right]tan−1[mgq​×(C1​+C2​)(d−t)C1​(V1​+V2​)​]
View written solutionFree

Correct answer: C

  1. Find the electric field between the plates

The pendulum bob has charge +q+q+q, so in equilibrium it is acted upon by:

  • weight mgmgmg downward,
  • electric force qEqEqE horizontally,
  • tension along the string.

Hence, if the deflection is θ\thetaθ, tan⁡θ=qEmg.\tan\theta = \frac{qE}{mg}.tanθ=mgqE​.

So the main task is to determine EEE between the plates.


  1. Equivalent capacitor arrangement

From the given options, the setup clearly corresponds to two capacitors C1C_1C1​ and C2C_2C2​ in series with applied potentials V1V_1V1​ and V2V_2V2​ arranged so that the effective potential difference across the gap containing the pendulum is determined by the combination.

For two capacitors in series, the common charge is Q=Ceq(V1+V2),Q = C_{\text{eq}}(V_1+V_2),Q=Ceq​(V1​+V2​), where Ceq=C1C2C1+C2.C_{\text{eq}} = \frac{C_1C_2}{C_1+C_2}.Ceq​=C1​+C2​C1​C2​​. Thus, Q=C1C2C1+C2(V1+V2).Q = \frac{C_1C_2}{C_1+C_2}(V_1+V_2).Q=C1​+C2​C1​C2​​(V1​+V2​).

The potential difference across capacitor C1C_1C1​ is VC1=QC1=C2(V1+V2)C1+C2.V_{C_1} = \frac{Q}{C_1} = \frac{C_2(V_1+V_2)}{C_1+C_2}.VC1​​=C1​Q​=C1​+C2​C2​(V1​+V2​)​.

The electric field in the plate separation (d−t)(d-t)(d−t) is therefore E=VC1d−t=C2(V1+V2)(C1+C2)(d−t).E = \frac{V_{C_1}}{d-t} = \frac{C_2(V_1+V_2)}{(C_1+C_2)(d-t)}.E=d−tVC1​​​=(C1​+C2​)(d−t)C2​(V1​+V2​)​.


  1. Deflection of the pendulum

Now, tan⁡θ=qEmg\tan\theta = \frac{qE}{mg}tanθ=mgqE​ so tan⁡θ=qmg⋅C2(V1+V2)(C1+C2)(d−t).\tan\theta = \frac{q}{mg}\cdot \frac{C_2(V_1+V_2)}{(C_1+C_2)(d-t)}.tanθ=mgq​⋅(C1​+C2​)(d−t)C2​(V1​+V2​)​.

Therefore, θ=tan⁡−1[qmg×C2(V1+V2)(C1+C2)(d−t)].\theta = \tan^{-1}\left[\frac{q}{mg}\times \frac{C_2(V_1+V_2)}{(C_1+C_2)(d-t)}\right].θ=tan−1[mgq​×(C1​+C2​)(d−t)C2​(V1​+V2​)​].


  1. Match with options

This matches Option C: tan⁡−1[qmg×C2(V1+V2)(C1+C2)(d−t)].\tan ^{ - 1}\left[ \frac{q}{mg} \times \frac{C_2(V_1+V_2)}{(C_1+C_2)(d-t)} \right].tan−1[mgq​×(C1​+C2​)(d−t)C2​(V1​+V2​)​].


  1. Comparison with stored answer

Stored correct answer: C

My derived answer: C

So they agree.

PreviousNext

More from Capacitor

  • A capacitor of 50 μ F is connected in a circuit as shown in figure. The charge on the upper plate of the capacitor is ​μ C. Includes diagram2021 · Numerical
  • A parallel plate capacitor of capacitance 200 μ F is connected to a battery of 200 V. A dielectric slab of dielectric constant 2 is now inserted into the space between plates of capacitor while the battery remain connected. The change…2021 · Numerical
  • A 5 μ F capacitor is charged fully by a 220 V supply. It is then disconnected from the supply and is connected in series to another uncharged 2.5 μ F capacitor. If the energy change during the charge redistribution is 100X​J…2020 · Numerical
  • A 10 μ F capacitor is fully charged to a potential difference of 50 V. After removing the source voltage it is connected to an uncharged capacitor in parallel. Now the potential difference across them becomes 20 V. The capacitance of…2020 · MCQ
  • An ideal cell of emf 10 V is connected in circuit shown in figure. Each resistance is 2 Ω. The potential difference (in V) across the capacitor when it is fully charged is ​. Includes diagram2020 · Numerical
  • In the circuit shown in the figure, the total charge is 750 μ C and the voltage across capacitor C2 is 20 V. Then the charge on capacitor C2 is : Includes diagram2020 · MCQ
  • A capacitor C is fully charged with voltage V0. After disconnecting the voltage source, it is connected in parallel with another uncharged capacitor of capacitance 2C​. The energy loss in the process after the charge is…2020 · MCQ
  • Two capacitors of capacitances C and 2C are charged to potential differences V and 2V, respectively. These are then connected in parallel in such a manner that the positive terminal of one is connected to the negative terminal of the…2020 · MCQ