An elastic string of unstretched length \(L\) and force constant \(k\) is stretched by a small length \(x\). It is further stretched by another small length \(y\). The work done in the second stretching is:
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Elastic string work:
\[
W = \frac{1}{2}k(x_2^2 - x_1^2)
\]
Always integrate tension over extension.