Lagrangian system
In mathematics, a Lagrangian system is a pair, consisting of a smooth fiber bundle and a Lagrangian density, which yields the Euler–Lagrange differential operator acting on sections of.
In classical mechanics, many dynamical systems are Lagrangian systems. The configuration space of such a Lagrangian system is a fiber bundle over the time axis. In particular, if a reference frame is fixed. In classical field theory, all field systems are the Lagrangian ones.
Lagrangians and Euler–Lagrange operators
A Lagrangian density of order is defined as an -form,, on the -order jet manifold of.A Lagrangian can be introduced as an element of the variational bicomplex of the differential graded algebra of exterior forms on jet manifolds of. The coboundary operator of this bicomplex contains the variational operator which, acting on, defines the associated Euler–Lagrange operator.
In coordinates
Given bundle coordinates on a fiber bundle and the adapted coordinates,, ) on jet manifolds, a Lagrangian and its Euler–Lagrange operator readwhere
denote the total derivatives.
For instance, a first-order Lagrangian and its second-order Euler–Lagrange operator take the form
Euler–Lagrange equations
The kernel of an Euler–Lagrange operator provides the Euler–Lagrange equations.Cohomology and Noether's theorems
of the variational bicomplex leads to the so-calledvariational formula
where
is the total differential and is a Lepage equivalent of. Noether's first theorem and Noether's second theorem are corollaries of this variational formula.