Fig (a) - Resistivity rT of copper as a function of temperature T
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In metallic alloys, the resistivity is very large, but has a weak temperature dependence, as seen in below figure.

Fig(b) - Resistivity rT
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of nichrome as a function of absolute temperature T
Alloys have a residual resistivity even at absolute zero, but a pure metal has a vanishingly small resistivity. This can be used to check the purity of metals.
The resistivity of a semiconductor decreases rapidly with increasing temperature as shown in fig (c).

Fig (c) - Temperature dependence of resistivity for a typical semiconductor
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This means that a is negative. The resistivity of an insulator too decreases exponentially with increase in temperature.
These observations may be understood qualitatively using the equation for
r.

Since m and e are constants,

In metals, the number of free electrons, n does not change with temperature. But, as temperature increases, the atoms/ions vibrate with increasing amplitude. Therefore, the collisions of electrons with them become more frequent, resulting in a decrease in
t. This means an increase in
r with increase in temperature.
In both insulators and semiconducotors, t remains almost constant, but the number of free charge carriers increases with temperature. At any temperature T, the number of carriers is given by
n(T) = n
0 exp (-E
g/k
B T)
where Eg is the energy gap between the conduction and valence bonds. From this, we can get the temperature dependence of r to be
r(t) = r
0 exp (E
g/k
B T)

In semiconductors, E
g ~ 1 eV,
\ r is not very high.
In insulators, Eg >> 1 eV; \ r is very high.
Also, this last equation shows that for semiconductors and insulators, resistivity increases with decreasing temperature.