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Electrostatics question

2023 · 10 Apr · Shift 1 · Q71
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Electrostatics question

2023 · 10 Apr · Shift 1 · Q71

JEE MainPhysicsElectrostaticsNumerical+4 / −1
Three concentric spherical metallic shells X, Y and Z of radius a, b and c respectively [a < b < c] have surface charge densities σ,−σ\sigma,-\sigmaσ,−σ and σ\sigmaσ respectively. The shells X and Z are at same potential. If the radii of X & Y are 2 cm and 3 cm, respectively. The radius of shell Z is ‾\underline{\hspace{2cm}}​ cm.
Numerical answer
View written solutionFree

Correct answer: 5

  1. Given data

Three concentric metallic spherical shells:

  • Shell XXX of radius aaa
  • Shell YYY of radius bbb
  • Shell ZZZ of radius ccc

with a<b<ca<b<ca<b<c.

Surface charge densities are respectively:

  • On XXX: σ\sigmaσ
  • On YYY: −σ-\sigma−σ
  • On ZZZ: σ\sigmaσ

Also given:

  • a=2 cma=2\text{ cm}a=2 cm
  • b=3 cmb=3\text{ cm}b=3 cm
  • Potentials of shells XXX and ZZZ are equal.

We need to find ccc.


  1. Charge on each shell

Since surface charge density is given, total charge on each shell is:

QX=4πa2σQ_X = 4\pi a^2\sigmaQX​=4πa2σ QY=−4πb2σQ_Y = -4\pi b^2\sigmaQY​=−4πb2σ QZ=4πc2σQ_Z = 4\pi c^2\sigmaQZ​=4πc2σ


  1. Potential at shell XXX

Potential due to a spherical shell:

  • At an external point: V=14πε0QrV = \dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{r}V=4πε0​1​rQ​
  • At any internal point/on inner region of shell: V=14πε0QRV = \dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{R}V=4πε0​1​RQ​ where RRR is shell radius.

At r=ar=ar=a (shell XXX):

  • Due to shell XXX itself: VXX=14πε0QXaV_{XX} = \frac{1}{4\pi\varepsilon_0}\frac{Q_X}{a}VXX​=4πε0​1​aQX​​
  • Due to shell YYY (point inside shell YYY): VYX=14πε0QYbV_{YX} = \frac{1}{4\pi\varepsilon_0}\frac{Q_Y}{b}VYX​=4πε0​1​bQY​​
  • Due to shell ZZZ (point inside shell ZZZ): VZX=14πε0QZcV_{ZX} = \frac{1}{4\pi\varepsilon_0}\frac{Q_Z}{c}VZX​=4πε0​1​cQZ​​

So,

VX=14πε0(QXa+QYb+QZc)V_X = \frac{1}{4\pi\varepsilon_0}\left(\frac{Q_X}{a}+\frac{Q_Y}{b}+\frac{Q_Z}{c}\right)VX​=4πε0​1​(aQX​​+bQY​​+cQZ​​)

Substitute charges:

VX=14πε0(4πa2σa+−4πb2σb+4πc2σc)V_X = \frac{1}{4\pi\varepsilon_0}\left(\frac{4\pi a^2\sigma}{a}+\frac{-4\pi b^2\sigma}{b}+\frac{4\pi c^2\sigma}{c}\right)VX​=4πε0​1​(a4πa2σ​+b−4πb2σ​+c4πc2σ​)

VX=14πε0(4πσ)(a−b+c)V_X = \frac{1}{4\pi\varepsilon_0}(4\pi\sigma)(a-b+c)VX​=4πε0​1​(4πσ)(a−b+c)


  1. Potential at shell ZZZ

At r=cr=cr=c:

  • Due to shell XXX: VXZ=14πε0QXcV_{XZ} = \frac{1}{4\pi\varepsilon_0}\frac{Q_X}{c}VXZ​=4πε0​1​cQX​​
  • Due to shell YYY: VYZ=14πε0QYcV_{YZ} = \frac{1}{4\pi\varepsilon_0}\frac{Q_Y}{c}VYZ​=4πε0​1​cQY​​
  • Due to shell ZZZ itself: VZZ=14πε0QZcV_{ZZ} = \frac{1}{4\pi\varepsilon_0}\frac{Q_Z}{c}VZZ​=4πε0​1​cQZ​​

Thus,

VZ=14πε0QX+QY+QZcV_Z = \frac{1}{4\pi\varepsilon_0}\frac{Q_X+Q_Y+Q_Z}{c}VZ​=4πε0​1​cQX​+QY​+QZ​​

Substitute charges:

VZ=14πε04πσ(a2−b2+c2)cV_Z = \frac{1}{4\pi\varepsilon_0}\frac{4\pi\sigma(a^2-b^2+c^2)}{c}VZ​=4πε0​1​c4πσ(a2−b2+c2)​

VZ=14πε0(4πσ)a2−b2+c2cV_Z = \frac{1}{4\pi\varepsilon_0}(4\pi\sigma)\frac{a^2-b^2+c^2}{c}VZ​=4πε0​1​(4πσ)ca2−b2+c2​


  1. Use condition VX=VZV_X = V_ZVX​=VZ​

Since shells XXX and ZZZ are at same potential,

a−b+c=a2−b2+c2ca-b+c = \frac{a^2-b^2+c^2}{c}a−b+c=ca2−b2+c2​

Multiply by ccc:

c(a−b+c)=a2−b2+c2c(a-b+c)=a^2-b^2+c^2c(a−b+c)=a2−b2+c2

Expand left side:

ac−bc+c2=a2−b2+c2ac-bc+c^2=a^2-b^2+c^2ac−bc+c2=a2−b2+c2

Cancel c2c^2c2 from both sides:

ac−bc=a2−b2ac-bc=a^2-b^2ac−bc=a2−b2

Factor both sides:

c(a−b)=(a−b)(a+b)c(a-b)=(a-b)(a+b)c(a−b)=(a−b)(a+b)

Since a≠ba\neq ba=b, divide by (a−b)(a-b)(a−b):

c=a+bc=a+bc=a+b


  1. Substitute values

c=2+3=5 cmc=2+3=5\text{ cm}c=2+3=5 cm


  1. Final answer

The radius of shell ZZZ is

5 cm\boxed{5\text{ cm}}5 cm​


  1. Comparison with stored answer

Stored correct answer: 555

Our derived answer is also 555, so it agrees.

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