If the normal strain is defined in reference to the final length, that is,
\[\epsilon_{n}^{\prime}=\lim _{p \rightarrow p^{\prime}}\left(\frac{\Delta s^{\prime}-\Delta s}{\Delta s^{\prime}}\right)\]
instead of in reference to the original length, Eq. $2-2,$ show that the difference in these strains is represented as a second-order term, namely, $\epsilon_{n}-\epsilon_{n}^{\prime}=\epsilon_{n} \epsilon_{n}^{\prime}.$