Euler–Lagrange equation

Creator
Creator
Seonglae ChoSeonglae Cho
Created
Created
2024 May 2 12:45
Editor
Edited
Edited
2025 Oct 6 23:6
By differentiating the scalar Lagrangian in the energy dimension with respect to the generalized coordinates and generalized velocities, excluding the constraints, the Euler-Lagrange equation is derived using the variational method.

Symmetry of physical laws under variation of the path in time

Principle of stationary action →
Euler–Lagrange equation

Conservation of Energy

For a static empty universe
However, our universe is not globally symmetric with respect to time since spacetime itself evolves. Global energy conservation does not hold, even though local conservation () still applies.

Contracted Bianchi identities

 
 
Euler–Lagrange equation
In the calculus of variations and classical mechanics, the Euler–Lagrange equations[1] are a system of second-order ordinary differential equations whose solutions are stationary points of the given action functional. The equations were discovered in the 1750s by Swiss mathematician Leonhard Euler and Italian mathematician Joseph-Louis Lagrange.
 
 
 

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