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Theorem

Noether's Second Theorem

Mathematical Physics

Noether's Second Theorem is a result of mathematics and theoretical physics, proved by Emmy Noether alongside her more widely known first theorem, relating the symmetries of an action functional that depend on arbitrary functions of position, rather than on constant parameters, to a system of differential identities among the equations of motion. It governs the local, or gauge, symmetries found in field theories such as general relativity and electromagnetism, in contrast to the global symmetries and conserved quantities covered by Noether's first theorem.

Facts
Statement
Whenever a Lagrangian admits gauge symmetries parametrized linearly by q arbitrary functions and their derivatives, there exist q linear differential relations among the Euler-Lagrange equations of that Lagrangian. 1
Proof Year
1918 1
Connections

Named After

Emmy Noether, Mathematicians

Derived from the theorem's own name (unambiguous possessive-token match to exactly one live mathematician entity, w-bfill-g5-0924 browse backfill)

Sources
1. Noether's second theorem, Wikipedia
  • Noether's second theorem section
    The statement of Noether's second theorem is that whenever given a Lagrangian L as above that admits gauge symmetries parametrized linearly by q arbitrary functions and their derivatives, then there exist q linear differential relations between the Euler-Lagrange equations of L.
  • References
    Invariante Variationsprobleme, Nachr. D. Konig. Gesellsch. D. Wiss. Zu Gottingen, Math-phys. Klasse, 1918: 235-257.
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