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Solved: If the normal strain is defined in reference to
Chapter 2, Problem 2-34(choose chapter or problem)
If the normal strain is defined in reference to the final length \(\Delta s^{\prime}\), that is,
\(\epsilon^{\prime}=\lim _{\Delta s^{\prime} \rightarrow 0}\left(\frac{\Delta s^{\prime}-\Delta s}{\Delta s^{\prime}}\right)\)
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, \(\epsilon-\epsilon^{\prime}=\epsilon \epsilon^{\prime}\).
Questions & Answers
QUESTION:
If the normal strain is defined in reference to the final length \(\Delta s^{\prime}\), that is,
\(\epsilon^{\prime}=\lim _{\Delta s^{\prime} \rightarrow 0}\left(\frac{\Delta s^{\prime}-\Delta s}{\Delta s^{\prime}}\right)\)
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, \(\epsilon-\epsilon^{\prime}=\epsilon \epsilon^{\prime}\).
ANSWER:Step 1 of 3
The normal strain in the reference to the final length is given as,
Here, is the final length and is the initial length.
The normal strain in the reference to the initial length is given as,