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Worked Examples · Example 2.5

Q.The electrical resistance of a column of 0.05 mol L−10.05\ mol\ L^{-1} NaOH solution of diameter 1 cm1\ cm and length 50 cm50\ cm is 5.55×1035.55 \times 10^{3} ohm. Calculate its resistivity, conductivity and molar conductivity.

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Using the cell constant derived from the column dimensions and the measured resistance, we find resistivity ρ=87.19 Ω cm\rho = 87.19\ \Omega\ \text{cm}, conductivity κ=0.011469 S cm−1\kappa = 0.011469\ \text{S cm}^{-1}, and molar conductivity Λm=229.4 S cm2 mol−1\Lambda_m = 229.4\ \text{S cm}^2\ \text{mol}^{-1}.

The key to solving this problem is understanding that resistance (RR) is a property of the entire sample, while resistivity (ρ\rho) and conductivity (κ\kappa) are intrinsic properties of the material. The geometry of the column — its length and cross-sectional area — acts as a bridge between them.

Think of it this way: a longer column offers more resistance (electrons have to travel further), and a wider column offers less resistance (more lanes for electrons to flow). The cell constant G∗G^* captures this geometry: G∗=lAG^* = \frac{l}{A}. Once you know G∗G^*, you can extract the material's intrinsic conductivity from the measured resistance using κ=G∗R\kappa = \frac{G^*}{R}.

Molar conductivity then extends this idea to account for concentration — it tells you how well a given amount of dissolved electrolyte conducts, making it possible to compare different solutions fairly.

Let’s work through it step by step.


  1. Find the cross-sectional area of the column.

    The column is cylindrical with diameter d=1 cmd = 1\ \text{cm}, so radius r=0.5 cmr = 0.5\ \text{cm}.

    Area A=πr2=π(0.5)2=0.25π cm2A = \pi r^2 = \pi (0.5)^2 = 0.25\pi\ \text{cm}^2.

    Numerically: A=0.25×3.1416≈0.7854 cm2A = 0.25 \times 3.1416 \approx 0.7854\ \text{cm}^2.

  2. Calculate the cell constant G∗G^*.

    The cell constant is defined as G∗=lAG^* = \frac{l}{A}, where l=50 cml = 50\ \text{cm} is the length between electrodes.

G∗=50 cm0.7854 cm2≈63.66 cm−1G^* = \frac{50\ \text{cm}}{0.7854\ \text{cm}^2} \approx 63.66\ \text{cm}^{-1}

Tip

The cell constant has units of cm−1\text{cm}^{-1} (or m−1\text{m}^{-1} in SI). It is a fixed value for a given conductivity cell geometry — you can think of it as the "geometric factor" that converts resistance into resistivity.

  1. Compute resistivity ρ\rho. Resistivity is related to resistance by ρ=R⋅Al=RG∗\rho = R \cdot \frac{A}{l} = \frac{R}{G^*}. Given R=5.55×103 ΩR = 5.55 \times 10^3\ \Omega,

ρ=5.55×10363.66≈87.19 Ω cm\rho = \frac{5.55 \times 10^3}{63.66} \approx 87.19\ \Omega\ \text{cm}

Watch out

A common mistake is to forget that ll and AA must be in consistent units. Here, using cm for length and cm² for area gives resistivity in Ω cm\Omega\ \text{cm}, which is standard for electrolyte solutions. If you used metres, you'd get Ω m\Omega\ \text{m} — both are correct, but the numerical value changes.

  1. Find conductivity κ\kappa. Conductivity is simply the reciprocal of resistivity: κ=1ρ\kappa = \frac{1}{\rho}.

κ=187.19≈0.011469 S cm−1\kappa = \frac{1}{87.19} \approx 0.011469\ \text{S cm}^{-1}

Alternatively, directly from the cell constant: κ=G∗R=63.665.55×103=0.011469 S cm−1\kappa = \frac{G^*}{R} = \frac{63.66}{5.55 \times 10^3} = 0.011469\ \text{S cm}^{-1}. Both routes give the same result.

  1. Calculate molar conductivity Λm\Lambda_m. …

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