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Electrostatics question

2024 · 27 Jan · Shift 1 · Q82
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Electrostatics question

2024 · 27 Jan · Shift 1 · Q82

JEE MainPhysicsElectrostaticsNumerical+4 / −1
A thin metallic wire having cross sectional area of 10−4 m210^{-4} \mathrm{~m}^210−4 m2 is used to make a ring of radius 30 cm30 \mathrm{~cm}30 cm. A positive charge of 2π C2 \pi \mathrm{~C}2π C is uniformly distributed over the ring, while another positive charge of 30 pC\mathrm{pC}pC is kept at the centre of the ring. The tension in the ring is ‾\underline{\hspace{2cm}}​N\mathrm{N}N; provided that the ring does not get deformed (neglect the influence of gravity). (given, 14πϵ0=9×109\frac{1}{4 \pi \epsilon_0}=9 \times 10^94πϵ0​1​=9×109 SI units)
Numerical answer
View written solutionFree

Correct answer: 3

  1. Given data
  • Cross-sectional area of wire: A=10−4 m2A = 10^{-4}\,\text{m}^2A=10−4m2
  • Radius of ring: R=30 cm=0.3 mR = 30\,\text{cm} = 0.3\,\text{m}R=30cm=0.3m
  • Charge uniformly distributed on ring: Q=2π CQ = 2\pi\,\text{C}Q=2πC
  • Charge at centre: q=30 pC=30×10−12 Cq = 30\,\text{pC} = 30\times 10^{-12}\,\text{C}q=30pC=30×10−12C
  • Coulomb constant: k=14πε0=9×109k = \dfrac{1}{4\pi\varepsilon_0} = 9\times 10^9k=4πε0​1​=9×109

We need the tension in the ring.


  1. Force on a small element of the ring due to the central charge

Let the linear charge density on the ring be

λ=Q2πR\lambda = \frac{Q}{2\pi R}λ=2πRQ​

A small element subtending angle dθd\thetadθ has length

dl=R dθdl = R\,d\thetadl=Rdθ

and charge

dq=λ dl=λR dθ=Q2πRR dθ=Q2πdθdq = \lambda\,dl = \lambda R\,d\theta = \frac{Q}{2\pi R}R\,d\theta = \frac{Q}{2\pi}d\thetadq=λdl=λRdθ=2πRQ​Rdθ=2πQ​dθ

The central charge qqq repels this element radially outward with force

dF=kq dqR2dF = \frac{kq\,dq}{R^2}dF=R2kqdq​

So,

dF=kqR2⋅Q2πdθdF = \frac{kq}{R^2}\cdot \frac{Q}{2\pi}d\thetadF=R2kq​⋅2πQ​dθ
  1. Relating this force to tension

Consider the small element of the ring subtending angle dθd\thetadθ.

If the tension in the ring is TTT, then the two tensions at its ends have resultant radial inward magnitude

2Tsin⁡dθ22T\sin\frac{d\theta}{2}2Tsin2dθ​

For small dθd\thetadθ,

sin⁡dθ2≈dθ2\sin\frac{d\theta}{2} \approx \frac{d\theta}{2}sin2dθ​≈2dθ​

Hence inward force due to tension is

2T⋅dθ2=T dθ2T\cdot \frac{d\theta}{2} = T\,d\theta2T⋅2dθ​=Tdθ

For equilibrium of the element,

T dθ=dFT\,d\theta = dFTdθ=dF

Therefore,

T dθ=kqR2⋅Q2πdθT\,d\theta = \frac{kq}{R^2}\cdot \frac{Q}{2\pi}d\thetaTdθ=R2kq​⋅2πQ​dθ

Cancelling dθd\thetadθ,

T=kqQ2πR2T = \frac{kqQ}{2\pi R^2}T=2πR2kqQ​
  1. Substitute values
T=(9×109)(30×10−12)(2π)2π(0.3)2T = \frac{(9\times 10^9)(30\times 10^{-12})(2\pi)}{2\pi(0.3)^2}T=2π(0.3)2(9×109)(30×10−12)(2π)​

The 2π2\pi2π cancels:

T=(9×109)(30×10−12)0.09T = \frac{(9\times 10^9)(30\times 10^{-12})}{0.09}T=0.09(9×109)(30×10−12)​

Now,

9×30=270,109×10−12=10−39\times 30 = 270, \qquad 10^9\times 10^{-12} = 10^{-3}9×30=270,109×10−12=10−3

So,

(9×109)(30×10−12)=270×10−3=0.27(9\times 10^9)(30\times 10^{-12}) = 270\times 10^{-3} = 0.27(9×109)(30×10−12)=270×10−3=0.27

Thus,

T=0.270.09=3 NT = \frac{0.27}{0.09} = 3\,\text{N}T=0.090.27​=3N
  1. Final answer

The tension in the ring is

3 N\boxed{3\,\text{N}}3N​

So the required integer is

3\boxed{3}3​
  1. Comparison with stored answer

Stored correct answer: 333

Our derived answer is also 333, so they agree.

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