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Electrostatics question

2023 · 30 Jan · Shift 2 · Q56
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Electrostatics question

2023 · 30 Jan · Shift 2 · Q56

JEE MainPhysicsElectrostaticsMCQ+4 / −1
As shown in the figure, a point charge QQQ is placed at the centre of conducting spherical shell of inner radius aaa and outer radius bbb. The electric field due to charge Q\mathrm{Q}Q in three different regions I,II\mathrm{I}, \mathrm{II}I,II and III\mathrm{III}III is given by: (I:r<a,II:a<r<b(\mathrm{I}: r \lt a, \mathrm{II}: a \lt r \lt b(I:r<a,II:a<r<b, III: r>br>br>b ) JEE Main 2023 (Online) 30th January Evening Shift Physics - Electrostatics Question 98 English
  1. A
    EI=0,EII=0,EIIIeq0E_I=0, E_{I I}=0, E_{I I I} eq 0EI​=0,EII​=0,EIII​eq0
  2. B
    EIeq0,EII=0,EIII=0E_I eq 0, E_{I I}=0, E_{III}=0EI​eq0,EII​=0,EIII​=0
  3. C
    EIeq0,EII=0,EIIIeq0E_I eq 0, E_{I I}=0, E_{III} eq 0EI​eq0,EII​=0,EIII​eq0
  4. D
    EI=0,EII=0,EIII=0E_I=0, E_{I I}=0, E_{I I I}=0EI​=0,EII​=0,EIII​=0
View written solutionFree

Correct answer: C

  1. Understand the setup

A point charge QQQ is placed at the centre of a conducting spherical shell.

  • Region I: r<ar<ar<a (inside the cavity)
  • Region II: a<r<ba<r<ba<r<b (inside the conducting material)
  • Region III: r>br>br>b (outside the shell)

We must determine whether the electric field is zero or non-zero in each region.


  1. Region I: r<ar<ar<a

This is the empty cavity containing the point charge at the centre.

Using Gauss's law for a spherical Gaussian surface of radius r<ar<ar<a:

∮E⃗⋅dA⃗=Qencε0\oint \vec E\cdot d\vec A = \frac{Q_{\text{enc}}}{\varepsilon_0}∮E⋅dA=ε0​Qenc​​

Since the point charge QQQ is enclosed,

E(4πr2)=Qε0E(4\pi r^2)=\frac{Q}{\varepsilon_0}E(4πr2)=ε0​Q​

So,

E=14πε0Qr2E=\frac{1}{4\pi\varepsilon_0}\frac{Q}{r^2}E=4πε0​1​r2Q​

Thus, in Region I,

EI≠0E_I\neq 0EI​=0


  1. Region II: a<r<ba<r<ba<r<b

This region lies inside the conducting material.

In electrostatic equilibrium, the electric field inside a conductor is always zero.

Therefore,

EII=0E_{II}=0EII​=0


  1. Region III: r>br>br>b

Outside the shell, consider a Gaussian surface of radius r>br>br>b.

The central charge QQQ induces:

  • charge −Q-Q−Q on the inner surface,
  • charge +Q+Q+Q on the outer surface, if the shell is initially neutral.

Total enclosed charge for r>br>br>b is:

Q+(−Q)+(+Q)=QQ+(-Q)+(+Q)=QQ+(−Q)+(+Q)=Q

Hence by Gauss's law,

E(4πr2)=Qε0E(4\pi r^2)=\frac{Q}{\varepsilon_0}E(4πr2)=ε0​Q​

So,

E=14πε0Qr2E=\frac{1}{4\pi\varepsilon_0}\frac{Q}{r^2}E=4πε0​1​r2Q​

Thus,

EIII≠0E_{III}\neq 0EIII​=0


  1. Compare with options
  • A: EI=0,EII=0,EIII≠0E_I=0, E_{II}=0, E_{III}\neq 0EI​=0,EII​=0,EIII​=0 ❌ since EI≠0E_I\neq 0EI​=0
  • B: EI≠0,EII=0,EIII=0E_I\neq 0, E_{II}=0, E_{III}=0EI​=0,EII​=0,EIII​=0 ❌ since EIII≠0E_{III}\neq 0EIII​=0
  • C: EI≠0,EII=0,EIII≠0E_I\neq 0, E_{II}=0, E_{III}\neq 0EI​=0,EII​=0,EIII​=0 ✅
  • D: EI=0,EII=0,EIII=0E_I=0, E_{II}=0, E_{III}=0EI​=0,EII​=0,EIII​=0 ❌

  1. Final answer

The correct option is:

C\boxed{\text{C}}C​

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