Second Variation: Euler-Lagrange Equation & \delta^2 S

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The discussion centers on the Euler-Lagrange equation and the concept of the second variation of a functional S, defined as \(\delta^2 S\). The first variation, \(\delta S = 0\), leads to the Euler-Lagrange equation, which is essential for determining the extremum of a functional. The second variation, \(\delta(\delta S) = 0\), is crucial for classifying whether a function \(q = q(t)\) represents a maximum or minimum in function space. The conversation highlights the importance of understanding both variations in the context of classical mechanics and variational calculus.

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Karlisbad
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Let be a functional S so [tex]\delta S =0[/tex] give the Euler-Lagrange equation where:

[tex]S= \int_{a}^{b}dtL(q,\dot q, t)[/tex]

My question is ..How the "second variation" [tex]\delta ( \delta S )=0= \delta ^{2} S[/tex] defined??.. in order we could decide if a function q=q(t) is either a maximum or a minimum point of function space..:confused: :confused: thanks.
 
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How's the "first variation" defined ?

Daniel.
 
The first variation of S (are you physicist..i say so because i use to see you in the QM forum :-p ) are the Euler-Lagrange equation defined via the functional derivative
 

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