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Electrostatics question

2016 · Shift 2 · Q54
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Electrostatics question

2016 · Shift 2 · Q54

JEE AdvancedPhysicsElectrostaticsMCQ+3 / −1
Consider an evacuated cylindrical chamber of height h having rigid conducting plates at the ends and an insulating curved surface as shown in the figure. A number of spherical balls made of a light weight and soft material and coated with a conducting material are placed on the bottom plate. The balls have a radius r << h. Now, a high voltage source (HV) connected across the conducting plates such that the bottom plate is at +V0 and the top plate at −-− V0. Due to their conducting surface, the balls will get charge, will become equipotential with the plate and are repelled by it. The balls will eventually collide with the top plate, where the coefficient of restitution can be taken to be zero due to the soft nature of the material of the balls. The electric field in the chamber can be considered to be that of a parallel plate capacitor. Assume that there are no collisions between the balls and the interaction between them is negligible. (Ignore gravity) JEE Advanced 2016 Paper 2 Offline Physics - Electrostatics Question 36 English The average current in the steady state registered by the ammeter in the circuit will be
  1. A
    proportional to V02V_0^2V02​
  2. B
    proportional to the potential V0{V_0}V0​
  3. C
    zero
  4. D
    proportions to V01/2V_0^{1/2}V01/2​
View written solutionFree

Correct answer: A

  1. Physical setup

    • Two rigid conducting plates are separated by height hhh.
    • The side surface is insulating.
    • Small light, soft, conducting-coated balls of radius rrr are placed on the lower plate.
    • A potential difference V0V_0V0​ is applied across the plates, so the electric field between plates is approximately uniform: E=V0hE = \frac{V_0}{h}E=hV0​​
  2. How current is produced

    Each ball acts like a charge carrier:

    • When touching the lower plate, it acquires charge.
    • It is then pulled upward by the electric field.
    • On touching the upper plate, it transfers charge there.
    • Then it may return and repeat the process.

    Thus, average current is I∼(charge carried per trip)×(number of trips per second)I \sim (\text{charge carried per trip}) \times (\text{number of trips per second})I∼(charge carried per trip)×(number of trips per second)

  3. Charge acquired by a ball

    A conducting sphere of radius rrr at potential VVV has charge of order q∼4πε0rVq \sim 4\pi \varepsilon_0 r Vq∼4πε0​rV

    Here the potential scale involved is of order V0V_0V0​, so q∝V0q \propto V_0q∝V0​

  4. Force on the charged ball

    Electric force on the ball is F=qEF = qEF=qE

    Since q∝V0q \propto V_0q∝V0​ and E=V0/h∝V0E = V_0/h \propto V_0E=V0​/h∝V0​, F∝V0⋅V0=V02F \propto V_0 \cdot V_0 = V_0^2F∝V0​⋅V0​=V02​

  5. Speed / time of flight

    The balls are light and soft, so we consider their motion under this electric force. For a given mass mmm and travel distance hhh, acceleration is a=Fm∝V02a = \frac{F}{m} \propto V_0^2a=mF​∝V02​

    Time to cross distance hhh under constant acceleration satisfies h∼12at2h \sim \frac{1}{2}at^2h∼21​at2 so t∝1a∝1V0t \propto \frac{1}{\sqrt{a}} \propto \frac{1}{V_0}t∝a​1​∝V0​1​

    Therefore, number of trips per second is f∝1t∝V0f \propto \frac{1}{t} \propto V_0f∝t1​∝V0​

  6. Average current

    Hence, I∝qf∝V0⋅V0=V02I \propto q f \propto V_0 \cdot V_0 = V_0^2I∝qf∝V0​⋅V0​=V02​

  7. Option check

    • A: proportional to V02V_0^2V02​ ✅
    • B: proportional to V0V_0V0​ ❌
    • C: zero ❌
    • D: proportional to V01/2V_0^{1/2}V01/2​ ❌

Therefore, the correct answer is A.

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