When a wire is stretched, the length of the wire will increase. At the same time, the wire will become thinner, that is, there is a decrease in the cross section of the wire. The ratio of change in diameter of the wire to the original diameter of the wire is known as lateral strain. The ratio of change in the length of the wire to the original length is known as longitudinal strain.
Within the elatic limit, the ratio of the lateral strain to the longitudinal strain is known as Poisson’s ratio.
Poisson’s ratio \quad \sigma \quad=\frac{\text { Lateral strain }}{\text { Longitudinal strain }}
\begin{aligned} \text { Lateral strain } & =\frac{\mathrm{d}}{D} \\ \text { Longitudinal strain } & =\frac{\mathrm{d} l}{l} \\ \sigma & =\frac{\mathrm{d} / D}{\mathrm{~d} l / l} \end{aligned}where d and dl are change in diameter and length respectively and D and l are original diameter and length respectively. If α and β are the longitudinal strain per unit stress and the lateral strain per unit stress respectively, then
\sigma=\frac{\beta}{\alpha}Poisson’s ratio has no units. The value of Poissons ratio depends on the nature of the material.
Read More Topics |
Factors affecting elasticity |
Three types of moduli elasticity |
Hooke’s law |