| Display title | Physics:Lagrangian (field theory) |
| Default sort key | Lagrangian (field theory) |
| Page length (in bytes) | 37,720 |
| Namespace ID | 3020 |
| Namespace | Physics |
| Page ID | 650107 |
| Page content language | en - English |
| Page content model | wikitext |
| Indexing by robots | Allowed |
| Number of redirects to this page | 0 |
| Counted as a content page | Yes |
| HandWiki item ID | None |
| Edit | Allow all users (infinite) |
| Move | Allow all users (infinite) |
| Page creator | imported>Steve2012 |
| Date of page creation | 04:00, 5 February 2024 |
| Latest editor | imported>Steve2012 |
| Date of latest edit | 04:00, 5 February 2024 |
| Total number of edits | 1 |
| Recent number of edits (within past 90 days) | 0 |
| Recent number of distinct authors | 0 |
Description | Content |
Article description: (description)
This attribute controls the content of the description and og:description elements. | Lagrangian field theory is a formalism in classical field theory. It is the field-theoretic analogue of Lagrangian mechanics. Lagrangian mechanics is used to analyze the motion of a system of discrete particles each with a finite number of degrees of freedom. Lagrangian field theory applies to continua... |
