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JEE Advanced 2016Paper 1
Exam
JEE Advanced
Year
2016
Paper
Paper 1
Subject
Physics
Chapter
Current Electricity

JEE Advanced 2016 · Paper 1 · Physics · Current Electricity

An infinite line charge of uniform electric charge density λ lies...

An infinite line charge of uniform electric charge density λ\lambda lies along the axis of an electrically conducting infinite cylindrical shell of radius R. At time t = 0, the space inside the cylinder is filled with a material of permittivity εε and electrical conductivity σ\sigma . The electrical conduction in the material follows Ohm's law.
Which one of the following graphs best describes the subsequent variation of the magnitude of current density j(t) at any point in the material?An infinite line charge of uniform electric charge density λ lies along the axis of an electrically conducting infiniteAn infinite line charge of uniform electric charge density λ lies along the axis of an electrically conducting infiniteAn infinite line charge of uniform electric charge density λ lies along the axis of an electrically conducting infiniteAn infinite line charge of uniform electric charge density λ lies along the axis of an electrically conducting infinite

Options

  1. AWhat is the unit of the Faraday constant (F) in the Nernst equation?
  2. BWhat is the unit of the Faraday constant (F) in the Nernst equation?
  3. CWhat is the unit of the Faraday constant (F) in the Nernst equation?
  4. DWhat is the unit of the Faraday constant (F) in the Nernst equation?

Correct answer

A. What is the unit of the Faraday constant (F) in the Nernst equation?

Step-by-step solution

This is the problem of RC circuit where the product RC is a constant.
So, due to leakage current, charge and current density will exponentially decay and will infinite time. So correct answer is A
For any small element
Resistance R = \dfrac{dr}{σ\left(2πrl\right)}
Capacitance C = \dfrac{ϵ2πrl}{dr}
Product R × C = \dfrac{ϵ}{σ} = constant
q = {q}_{0}{e}^{- \left(\dfrac{tσ}{ϵ}\right)}
I = \dfrac{dq}{dt} = \dfrac{{q}_{0}σ}{ϵ}{e}^{- \left(\dfrac{tσ}{ϵ}\right)}
Current density = \dfrac{I}{A} = \dfrac{{q}_{0}\dfrac{σ}{ϵ}{e}^{- \dfrac{tσ}{ϵ}}}{2πrl}
j\infty{e}^{- \dfrac{tσ}{ϵ}}
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