NVAMediumJEE 2026Coulomb's Law & Superposition Principle

JEE Physics 2026 Question with Solution

A point charge q=1μCq = 1\,\mu C is located at a distance 2cm2\,cm from one end of a thin insulating wire of length 10cm10\,cm having a charge Q=24μCQ = 24\,\mu C, distributed uniformly along its length, as shown in the figure. Force between qq and wire is _____ N.

(Use: 14πε0=9×109Nm2/C2\dfrac{1}{4\pi\varepsilon_0} = 9 \times 10^9\,N\cdot m^2/C^2)

Answer

Correct answer:90

Step-by-step solution

Standard Method

Given: Point charge q=1×106Cq = 1 \times 10^{-6} \, \text{C}, wire length L=0.10mL = 0.10 \, \text{m}, total charge on wire Q=24×106CQ = 24 \times 10^{-6} \, \text{C}, nearest end distance 0.02m0.02 \, \text{m}, and

14πε0=9×109N m2/C2\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9 \, \text{N m}^2/\text{C}^2

Find: Force between the point charge and the uniformly charged wire.

Step 1: Find linear charge density of the wire.

λ=QL=24×1060.10=2.4×104C/m\lambda = \frac{Q}{L} = \frac{24 \times 10^{-6}}{0.10} = 2.4 \times 10^{-4} \, \text{C/m}

Step 2: Consider an element of wire. Let an element dxdx be at a distance xx from the point charge.

dq=λdxdq = \lambda \, dx

Step 3: Write expression for force due to the element.

dF=14πε0qdqx2=9×109qλx2dxdF = \frac{1}{4\pi\varepsilon_0} \frac{q \, dq}{x^2} = 9 \times 10^9 \frac{q\lambda}{x^2} \, dx

Step 4: Set limits of integration. The nearest end is at x=0.02mx = 0.02 \, \text{m} and the far end is at x=0.12mx = 0.12 \, \text{m}.

Step 5: Integrate to find total force.

F=9×109qλ0.020.12dxx2F = 9 \times 10^9 \, q\lambda \int_{0.02}^{0.12} \frac{dx}{x^2} F=9×109×(1×106)×(2.4×104)[1x]0.020.12F = 9 \times 10^9 \times (1 \times 10^{-6}) \times (2.4 \times 10^{-4}) \left[ -\frac{1}{x} \right]_{0.02}^{0.12} F=9×109×2.4×1010(10.0210.12)F = 9 \times 10^9 \times 2.4 \times 10^{-10} \left( \frac{1}{0.02} - \frac{1}{0.12} \right) F=2.16×(508.33)90NF = 2.16 \times (50 - 8.33) \approx 90 \, \text{N}

Therefore, the force between the point charge and the wire is 90N90 \, \text{N}.

Integration Setup Explained

Given: The wire carries uniform charge, so the appropriate method is to divide it into small charge elements and add their Coulomb forces.

Because the wire is collinear with the point charge, all elemental forces act along the same line, so their magnitudes can be integrated directly.

For an element at distance xx,

dq=λdxdq = \lambda \, dx

and

dF=kqdqx2dF = k \frac{q \, dq}{x^2}

where

k=9×109N m2/C2k = 9 \times 10^9 \, \text{N m}^2/\text{C}^2

Substituting dq=λdxdq = \lambda dx gives

dF=9×109qλx2dxdF = 9 \times 10^9 \frac{q\lambda}{x^2} \, dx

The wire begins 0.02m0.02 \, \text{m} from the charge and ends at

0.02+0.10=0.12m0.02 + 0.10 = 0.12 \, \text{m}

So,

F=9×109qλ0.020.12x2dxF = 9 \times 10^9 q\lambda \int_{0.02}^{0.12} x^{-2} \, dx

Using

x2dx=1x\int x^{-2} \, dx = -\frac{1}{x}

we obtain the same final value,

F90NF \approx 90 \, \text{N}

Hence, the numerical answer is 90.

Common mistakes

  • Taking the far end distance as 0.10m0.10 \, \text{m} instead of 0.12m0.12 \, \text{m} is incorrect because the wire starts 0.02m0.02 \, \text{m} away from the charge. Always add the offset distance to the rod length before setting the upper limit.

  • Using F=kqQr2F = k\frac{qQ}{r^2} for the entire wire as if all its charge were concentrated at one point is wrong because different parts of the wire are at different distances from the point charge. Use integration with dq=λdxdq = \lambda dx instead.

  • Forgetting to convert μC\mu C to C\text{C} and cmcm to m\text{m} gives a force off by large powers of 1010. Convert all quantities to SI units before substitution.

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