MCQMediumJEE 2025Gauss's Law Applications

JEE Physics 2025 Question with Solution

A small bob of mass 100mg100 \, \text{mg} and charge +10μC+10 \, \mu\text{C} is connected to an insulating string of length 1m1 \, \text{m}. It is brought near to an infinitely long non-conducting sheet of charge density σ\sigma as shown in figure. If the string subtends an angle of 4545^\circ with the sheet at equilibrium, the charge density of sheet will be :

  • A

    0.885nC/cm20.885 \, \text{nC/cm}^2

  • B

    17.7nC/cm217.7 \, \text{nC/cm}^2

  • C

    885nC/cm2885 \, \text{nC/cm}^2

  • D

    1.77nC/cm21.77 \, \text{nC/cm}^2

Answer

Correct answer:D

Step-by-step solution

Standard Method

Given: Mass of bob m=100×106kgm = 100 \times 10^{-6} \, \text{kg}, charge q=10×106Cq = 10 \times 10^{-6} \, \text{C}, angle with the sheet θ=45\theta = 45^\circ, and for an infinite non-conducting sheet the electric field is

E=σ2ϵ0E = \frac{\sigma}{2\epsilon_0}

Find: The surface charge density σ\sigma.

At equilibrium, the bob is under three forces: weight mgmg downward, electrostatic force Fe=qEF_e = qE perpendicular to the sheet, and tension along the string. Since the string makes an angle of 4545^\circ, the horizontal and vertical balance gives

Tsinθ=FeT\sin\theta = F_e

and

Tcosθ=mgT\cos\theta = mg

Dividing the two equations,

tanθ=Femg\tan\theta = \frac{F_e}{mg}

Using Fe=qE=qσ2ϵ0F_e = qE = q\frac{\sigma}{2\epsilon_0},

tanθ=qσ2mgϵ0\tan\theta = \frac{q\sigma}{2mg\epsilon_0}

So,

σ=2mgϵ0tanθq\sigma = \frac{2mg\epsilon_0\tan\theta}{q}

Substitute the values from the solution:

σ=2×(100×106)×10×(8.85×1012)×110×106\sigma = \frac{2 \times (100 \times 10^{-6}) \times 10 \times (8.85 \times 10^{-12}) \times 1}{10 \times 10^{-6}}

Since tan45=1\tan 45^\circ = 1,

σ=1.77×109C/m2\sigma = 1.77 \times 10^{-9} \, \text{C/m}^2

This is written in the source solution as 1.77nC/cm21.77 \, \text{nC/cm}^2.

Therefore, the correct option is D.

Force Balance in Detail

Given: The sheet produces a uniform electric field perpendicular to its surface. The positively charged bob experiences repulsion, so the electric force is horizontal while gravity acts vertically downward.

Find: σ\sigma using equilibrium of forces.

Resolve tension TT into components:

  • Horizontal component: TsinθT\sin\theta
  • Vertical component: TcosθT\cos\theta

Equilibrium requires

Tsinθ=qET\sin\theta = qE

and

Tcosθ=mgT\cos\theta = mg

Now divide the equations to eliminate TT:

TsinθTcosθ=qEmg\frac{T\sin\theta}{T\cos\theta} = \frac{qE}{mg}

Hence,

tanθ=qmgσ2ϵ0\tan\theta = \frac{q}{mg}\cdot \frac{\sigma}{2\epsilon_0}

Therefore,

σ=2mgϵ0tanθq\sigma = \frac{2mg\epsilon_0\tan\theta}{q}

Putting m=100×106kgm = 100 \times 10^{-6} \, \text{kg}, g=10m/s2g = 10 \, \text{m/s}^2, ϵ0=8.85×1012\epsilon_0 = 8.85 \times 10^{-12}, q=10×106Cq = 10 \times 10^{-6} \, \text{C}, and θ=45\theta = 45^\circ,

σ=2×100×106×10×8.85×101210×106\sigma = \frac{2 \times 100 \times 10^{-6} \times 10 \times 8.85 \times 10^{-12}}{10 \times 10^{-6}} σ=1770×1012C/m2=1.77×109C/m2\sigma = 1770 \times 10^{-12} \, \text{C/m}^2 = 1.77 \times 10^{-9} \, \text{C/m}^2

So the answer matches option D as concluded in the solution.

Common mistakes

  • Using Fe=mgF_e = mg directly without resolving the tension is incorrect in general. That shortcut works here only because θ=45\theta = 45^\circ makes the horizontal and vertical force balances equal in magnitude. Always write both equilibrium equations first.

  • Taking the electric field of an infinite non-conducting sheet as E=σϵ0E = \frac{\sigma}{\epsilon_0} is wrong. For a single infinite non-conducting sheet, the correct field is E=σ2ϵ0E = \frac{\sigma}{2\epsilon_0}.

  • Confusing the angle with the sheet and the angle with the vertical can lead to wrong trigonometric ratios. Since the sheet is vertical, the given 4545^\circ is also the angle with the vertical here, so use consistent components while resolving tension.

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