What does the square of a differential mean?

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SUMMARY

The discussion focuses on the mathematical interpretation of the square of a differential in the context of calculating the elastic potential energy of a spring under gravity. The integral involves the term ##d\xi^2##, which is not typical since the square of a differential is generally considered to be zero. However, the participants clarify that in this scenario, the square of the differential has unique properties that contribute to the overall calculation. The effective spring constant, denoted as ##k'##, plays a crucial role in evaluating the integral, which ultimately leads to the expression for potential energy.

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  • Understanding of calculus, specifically integrals and differentials.
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  • Knowledge of spring constants and their significance in mechanics.
  • Basic grasp of infinitesimal calculus and limits.
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  • Study the derivation of elastic potential energy in springs using calculus.
  • Learn about the properties of differentials and their applications in physics.
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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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