Lagrangian system

A Lagrangian density L (or, simply, a Lagrangian) of order r is defined as an n-form, n = dim X, on the r-order jet manifold J^rY of Y.

A Lagrangian L can be introduced as an element of the variational bicomplex of the differential graded algebra O^∗_∞(Y) of exterior forms on jet manifolds of Y → X. The coboundary operator of this bicomplex contains the variational operator δ which, acting on L, defines the associated Euler–Lagrange operator δL.

Given bundle coordinates x^λ, yⁱ on a fiber bundle Y and the adapted coordinates x^λ, yⁱ, yⁱ_Λ, (Λ = (λ₁, ...,λ_k), |Λ| = k ≤ r) on jet manifolds J^rY, a Lagrangian L and its Euler–Lagrange operator read

${\displaystyle L={\mathcal {L}}(x^{\lambda },y^{i},y_{\Lambda }^{i})\,d^{n}x,}$ 

${\displaystyle \delta L=\delta _{i}{\mathcal {L}}\,dy^{i}\wedge d^{n}x,\qquad \delta _{i}{\mathcal {L}}=\partial _{i}{\mathcal {L}}+\sum _{|\Lambda |}(-1)^{|\Lambda |}\,d_{\Lambda }\,\partial _{i}^{\Lambda }{\mathcal {L}},}$ 

where

${\displaystyle d_{\Lambda }=d_{\lambda _{1}}\cdots d_{\lambda _{k}},\qquad d_{\lambda }=\partial _{\lambda }+y_{\lambda }^{i}\partial _{i}+\cdots ,}$ 

denote the total derivatives.

For instance, a first-order Lagrangian and its second-order Euler–Lagrange operator take the form

${\displaystyle L={\mathcal {L}}(x^{\lambda },y^{i},y_{\lambda }^{i})\,d^{n}x,\qquad \delta _{i}L=\partial _{i}{\mathcal {L}}-d_{\lambda }\partial _{i}^{\lambda }{\mathcal {L}}.}$ 

The kernel of an Euler–Lagrange operator provides the Euler–Lagrange equations δL = 0.

Cohomology of the variational bicomplex leads to the so-called variational formula

${\displaystyle dL=\delta L+d_{H}\Theta _{L},}$ 

where

${\displaystyle d_{H}\Theta _{L}=dx^{\lambda }\wedge d_{\lambda }\phi ,\qquad \phi \in O_{\infty }^{*}(Y)}$ 

is the total differential and θ_L is a Lepage equivalent of L. Noether's first theorem and Noether's second theorem are corollaries of this variational formula.

Extended to graded manifolds, the variational bicomplex provides description of graded Lagrangian systems of even and odd variables.^[1]

In a different way, Lagrangians, Euler–Lagrange operators and Euler–Lagrange equations are introduced in the framework of the calculus of variations.

In classical mechanics equations of motion are first and second order differential equations on a manifold M or various fiber bundles Q over ${\displaystyle \mathbb {R} }$ . A solution of the equations of motion is called a motion.^[2][3]

• Lagrangian mechanics
• Calculus of variations
• Noether's theorem
• Noether identities
• Jet bundle
• Jet (mathematics)
• Variational bicomplex

• Arnold, V. I. (1989), Mathematical Methods of Classical Mechanics, Graduate Texts in Mathematics, vol. 60 (second ed.), Springer-Verlag, ISBN 0-387-96890-3
• Giachetta, G.; Mangiarotti, L.; Sardanashvily, G. (1997). New Lagrangian and Hamiltonian Methods in Field Theory. World Scientific. ISBN 981-02-1587-8.
• Giachetta, G.; Mangiarotti, L.; Sardanashvily, G. (2011). Geometric formulation of classical and quantum mechanics. World Scientific. doi:10.1142/7816. hdl:11581/203967. ISBN 978-981-4313-72-8.
• Olver, P. (1993). Applications of Lie Groups to Differential Equations (2 ed.). Springer-Verlag. ISBN 0-387-94007-3.
• Sardanashvily, G. (2013). "Graded Lagrangian formalism". Int. J. Geom. Methods Mod. Phys. 10 (5). World Scientific: 1350016. arXiv:1206.2508. doi:10.1142/S0219887813500163. ISSN 0219-8878.

• Sardanashvily, G. (2009). "Fibre Bundles, Jet Manifolds and Lagrangian Theory. Lectures for Theoreticians". arXiv:0908.1886. Bibcode:2009arXiv0908.1886S. {{cite journal}}: Cite journal requires |journal= (help)