What does the square of a differential mean?

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The discussion centers on the integral used to calculate the elastic potential energy of a spring under compression, specifically addressing the implications of squaring a differential term. While the square of a differential is typically considered to be zero, in this context, it is argued that it has unique properties that contribute to the integral's evaluation. The participants suggest redefining the compression of a segment of the spring and evaluating the potential energy expression before taking the limit as the segment length approaches zero. This approach clarifies the role of the squared differential in the integral. Understanding this concept is crucial for accurately computing the potential energy in such scenarios.
Leo Liu
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When I was following the calculations of finding the potential energy of a spring standing on a table under gravity, I encountered the integral shown below, where ##d\xi## is the compression of a tiny segment of the spring and ##k'## is the effective spring constant of that segment. The integral sums up the elastic potential energy of each segment along the spring. However, it is not a run of the mill integral in that its differential term is squared. From my experience, the square of a differential is 0, but in this case it obviously possesses some unique properties. Could someone explain why this makes sense? And how do you compute this integral?
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Origin: https://www.zhihu.com/question/324405110/answer/1860254582
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From your text
k'=A(dx)^{-1} though I am not familiar at all with such a treatment of infinitesimal. Anyway
d\xi=B(dx)
k'(d\xi^2)=C dx
So
\int Dk'(d\xi^2)= \int E dx
as we expect.
 
I don't think it's helpful to think of it as a square differential. Let's call u(x) the compression of a segment of length δx. Then
u(x) = λg(L0-x)δx/kL0
k' = kL0/δx
Evaluate 1/2 k'u(x)2, and THEN (only then) let δx → 0. That's when it becomes a differential.
 
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