We know that, R = \(p\frac{l}{A}\)
If I = 1, A = 1 ⇒ P = R
Thus, resistivity of a material is numerically equal to the resistance of the conductor having unit length and unit cross-sectional area.
The resistivity of a material is found to be dependent on the temperature. Different materials do not exhibit the same dependence on temperature. Over a limited range of temperatures, that is not too large, the resistivity of a metallic conductor is approximately given by,
PT = P0[1 + a(T - T0)] .....(i)
Where ρT is the resistivity at a temperature T and ρ0 is the same at a reference temperature T0, α is called the temperature co-efficient of resistivity.
Relation (i) implies that a graph of ρT plotted against T would be a straight line. At temperatures much lower than 0°C, the graph, however, deviates considerably from a straight line (Fig.).

Resistivity ρT of metallic conductor as a function of temperature T