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NCERT Exemplar · Q50

Q.Conductivity κ\kappa, is equal to ____________. (Two or more than two options may be correct.)

(i) 1RlA\frac{1}{R}\frac{l}{A}
(ii) G∗R\frac{G^*}{R}
(iii) Λm\Lambda_m
(iv) lA\frac{l}{A}
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Conductivity κ\kappa is the reciprocal of resistivity, so it equals 1R⋅lA\frac{1}{R} \cdot \frac{l}{A} and also G∗R\frac{G^*}{R} (where G∗G^* is the cell constant). Options (i) and (ii) are correct; (iii) and (iv) are not.

The key here is to remember what conductivity actually means physically. Conductivity (κ\kappa) is a measure of how easily a solution conducts electricity — it’s the conductance of a 1 cm cube of the solution. That’s the intuitive picture: imagine a cube of the electrolyte, 1 cm on each side; the conductance you measure across opposite faces is the conductivity.

Now, how do we get there from measurable quantities? In the lab, you measure resistance RR of a solution placed in a cell with two electrodes of area AA separated by distance ll. The relationship between resistance and the geometry is:

R=ρlAR = \rho \frac{l}{A}

where ρ\rho is resistivity. Since conductivity is the reciprocal of resistivity:

κ=1ρ=1R⋅lA\kappa = \frac{1}{\rho} = \frac{1}{R} \cdot \frac{l}{A}

That’s option (i) directly.

But there’s a practical twist. In a real conductivity cell, you rarely know ll and AA separately — instead, you calibrate the cell and determine its cell constant G∗=lAG^* = \frac{l}{A}. So the same formula becomes:

κ=G∗R\kappa = \frac{G^*}{R}

That’s option (ii).

Now let’s check the others:

  1. Option (i): 1RlA\frac{1}{R}\frac{l}{A} — This is exactly the definition from R=ρlAR = \rho \frac{l}{A} and κ=1/ρ\kappa = 1/\rho. So this is correct.

  2. Option (ii): G∗R\frac{G^*}{R} — Since G∗=l/AG^* = l/A, this is just a repackaging of (i). Also correct. …

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