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Exercises · 3.4

Q.A negligibly small current is passed through a wire of length 15 m15\ \text{m} and uniform cross-section 6.0×10−7 m26.0 \times 10^{-7}\ \text{m}^2, and its resistance is measured to be 5.0 Ω5.0\ \Omega. What is the resistivity of the material at the temperature of the experiment?

Puducherry CbseNCERTSubjective· 2mImportance★★★★★
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Using the relation R=ρLAR = \rho \frac{L}{A}, the resistivity is found by rearranging to ρ=RAL\rho = \frac{RA}{L}. Substituting the given values gives ρ=2.0×10−7 Ω⋅m\rho = 2.0 \times 10^{-7}\ \Omega \cdot \text{m}.

The key idea here is that resistance depends on both the material's intrinsic property (resistivity) and the geometry of the wire. When we pass a negligibly small current, we avoid heating the wire, so the measurement is at the ambient temperature — exactly what the question asks for.

Why this approach works:

For a uniform conductor, resistance RR is directly proportional to length LL and inversely proportional to cross-sectional area AA. The constant of proportionality is the resistivity ρ\rho, a material property that changes with temperature. Since the current is tiny, Joule heating is negligible, so the measured resistance corresponds to the temperature of the experiment. We simply plug into the formula.

Let’s work through it step by step.

  1. Write the fundamental relation For a wire of uniform cross-section,

R=ρLAR = \rho \frac{L}{A}

This is the standard formula — memorize it. Resistivity ρ\rho has units Ω⋅m\Omega \cdot \text{m}.

  1. Rearrange for resistivity Multiply both sides by AA and divide by LL:

ρ=RAL\rho = \frac{R A}{L}

  1. Substitute the given values

    • R=5.0 ΩR = 5.0\ \Omega
    • A=6.0×10−7 m2A = 6.0 \times 10^{-7}\ \text{m}^2
    • L=15 mL = 15\ \text{m}

    So

ρ=(5.0)×(6.0×10−7)15\rho = \frac{(5.0) \times (6.0 \times 10^{-7})}{15}

  1. Simplify step by step First multiply numerator: 5.0×6.0×10−7=30×10−7=3.0×10−65.0 \times 6.0 \times 10^{-7} = 30 \times 10^{-7} = 3.0 \times 10^{-6} …

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