A metallic wire of length $L$ is fixed between two rigid supports. If the wire is cooled through a temperature difference $\Delta T$ ($Y$ = young’s modulus, $\rho$ = density, $\alpha$ = coefficient of linear expansion) then the frequency of transverse vibration is proportional to : 
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Tension in the string is developed in the wire due to cooling. The compression due to cooling is balanced by the expansion due to tension generated. Thus

$\frac{F L}{A Y}=L \alpha \Delta T$

$\Longrightarrow$ tension $F=Y A \alpha \Delta T$

Frequency of vibration is given as $f=\frac{1}{2 L} \sqrt{\frac{F}{\mu}}$

$\Longrightarrow f \propto \sqrt{\frac{Y A \alpha \Delta T}{\mu}}$

since $\rho A L=\mu L$

$f \propto \sqrt{\frac{Y \alpha}{\rho}}$

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