View source for Euler-Lagrange equations

The '''Euler-Lagrange equations''' are the differential equations that describe the conditions for a path through configuration space to make the action stationary — the mathematical core of [[Lagrangian mechanics]]. Given a Lagrangian L(q, dq/dt, t), where q represents generalized coordinates, the Euler-Lagrange equations state that the physical trajectory satisfies a specific second-order differential condition for each coordinate. Solutions to these equations are the actual paths taken by physical systems.

The equations were developed independently by Leonhard Euler (in the context of the [[Calculus of variations|calculus of variations]]) and Joseph-Louis Lagrange in the eighteenth century. Their derivation rests on a single insight: that infinitesimal variations away from the physical path produce no first-order change in the action, which is the [[Variational principle|variational principle]] in its most general form. This principle, that nature follows extremal paths, appears throughout physics in forms ranging from [[Fermat's principle|Fermat's principle of least time]] in optics to the [[Path integral formulation|path integral formulation]] of quantum mechanics.

''That the same mathematical structure — a variational condition on an action — governs light bending around a lens and an electron tunneling through a barrier is not a coincidence. It is a clue about the deep structure of physical law that we have not yet fully decoded.''

[[Category:Mathematics]]
[[Category:Physics]]