If the normal strain is defined in reference to the final length s', that is, instead of

If the normal strain is defined in reference to the final length ˆ†s', that is,

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, ε €“ ε€™ = ε ε€™.

Transcribed Image Text:

As' – As\ As' lim As'-0 e'