Question about derivation of Euler-Lagrange eq.

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Discussion Overview

The discussion revolves around the derivation of the Euler-Lagrange equation, specifically focusing on the necessary condition for the action to have a minimum, as presented in Landau & Lifschitz Mechanics. Participants explore the concept of first variations and their relationship to derivatives in the context of calculus and minimization principles.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant expresses confusion about why the first variation of the action must be zero for it to be at a minimum, seeking both a definition and an intuitive explanation.
  • Another participant suggests that the condition is analogous to the ordinary derivative being zero at a minimum of a function, implying that the action must remain unchanged by small variations near the minimum.
  • A different participant questions the analogy, noting that while the derivative is zero at a minimum, the function value at a small variation from the minimum is not necessarily equal to the minimum value.
  • One participant explains that at a minimum, moving in either direction results in an increase in function value, leading to a change in sign of the derivative, which must be zero at the minimum point.
  • Another participant posits that the first-order variation in the action being zero is equivalent to stating that the derivative of the action is zero at a minimum, suggesting that the terms can be used interchangeably in this context.
  • A later reply reinforces this equivalence, arguing that the terminology used is not merely fancy but accurately describes the condition for a minimum.
  • One participant provides a resource on functional derivatives, suggesting it may help clarify the topic further.

Areas of Agreement / Disagreement

Participants exhibit some agreement on the relationship between first variations and derivatives at a minimum, but there remains disagreement regarding the clarity and implications of the analogy. The discussion does not reach a consensus on the intuitive understanding of these concepts.

Contextual Notes

Some participants reference basic calculus principles, indicating a potential gap in understanding the relationship between variations and derivatives, but do not resolve the underlying confusion about these concepts.

Agrasin
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I've attached the part from Landau & Lifschitz Mechanics where I got confused.

"The necessary condition for S(action) to have a minimum (extremum) is that these terms (called the first variation, or simply the variation, of the integral) should be zero. "

Why is this a necessary condition? If you could point me towards a definition AND explain intuitively that'd be great.

(Background: I've learned calculus and Taylor expansions-- I think this is related. But, visually, I don't see why a variation in the function at the minimum should be zero. Imagine a paraboloid. The bottom is the minimum. If you go a tiny bit in any direction (a variation) then the first-order change in the function is NOT zero. Maybe it's just that I don't understand what first-order change means.)
 

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It's just saying that if it is a minimum then it has to be at the bottom of a bowl, so to speak. Just as the ordinary derivative of a function has to be zero at the function's minimum, so to does the action have to be unchanged by small variations in the path near the minimum of the action.
 
"Just as the ordinary derivative of a function has to be zero at the function's minimum, so to does the action have to be unchanged by small variations in the path near the minimum of the action."

Okay, please explain this analogy. I agree that the derivative of a function is zero at a minimum. But f(x+h) for any small variation h is NOT equal to f(x) necessarily. In fact, at a minimum, f(x+h) > f(x).
 
For simplicity, let's just deal with the 2-dimensional case. It's true that at the minimum, whichever way you go, you will always 'go up the hill' (so to speak). Hence, it's obvious that f(x-h) >f(x); and f(x+h) >f(x) (for any small variation h). So visually, the graph decreases as it goes from x-h to x, and it increases as it goes from x to x+h. In calculus, when a function decreases, it'll have a negative slope, which means that its derivative is negative. Similarly, when a function increases, it'll have a positive slope, which means that its derivative is positive. And since the derivative changes sign (from negative to positive) at the minimum point as the function goes from x-h to x + h, the derivative must be zero at this minimum point. All of this is the basic idea behind the first derivative test in calculus. So I would suggest you to refresh your mind a bit on calculus 101 because that will probably clear up all your confusion.

Once you understand what I've said above, then you can easily apply it to the case of minimizing the action in 3-dimensional coordinate. The idea is just the same!
 
So "the first order variation in S (action) has to be zero for S to be at a minimum" is just a fancy way of saying "the derivative of S is zero at a minimum"?
 
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Agrasin said:
So "the first order variation in S (action) has to be zero for S to be at a minimum" is just a fancy way of saying "the derivative of S is zero at a minimum"?

Well, I think you got it. You can re-write the quote by just replacing the word 'variation' with the word 'derivative' (because they mean basically the same thing as far as differentiation is concerned). In other words: "the first-order [derivative] in S (action) has to be zero for S to be at a minimum". It is totally not a fancy way of saying things, because it describes exactly what a minimum is.
 
It may help to read a little about functional derivatives: http://www.physics.byu.edu/faculty/berrondo/wt752/functional%20derivative.pdf
 
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