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The Euler-Lagrange expression and degenerate lagrange densities

Published online by Cambridge University Press:  09 April 2009

D. Lovelock
Affiliation:
Department of Applied MathematicsUniversity of WaterlooWaterloo, Ontario, Canada
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It is well known that many of the field equations from theoretical physics (e.g. Einstein field equations, Maxwell's equations, Klein-Gordon equation) can be obtained from a variational principle with a suitably chosen Lagrange density. In the case of the Einstein equations the corresponding Lagrangian is degenerate (i.e., the associated Euler-Lagrange equations are of second order whereas in general these would be of fourth order), while in the cases of the Maxwell and Klein-Gordon equations the Lagrangian usually used is not degenerate.

Type
Research Article
Copyright
Copyright © Australian Mathematical Society 1972

References

[1]Edelen, D. G. B., ‘The null set of the Euler-Lagrange operator’, Arch. Rational Mech. Anal. 11 (1962), 117121.CrossRefGoogle Scholar
[2]Lovelock, D., ‘The uniqueness of the Einstein field equations in a four dimensional space’, Arch. Rational Mech. Anal. 33, (1969), 5470.Google Scholar
[3]Lovelock, D., ‘Divergence-free tensorial concomitants’, Aequationes Mathematicae 4 (1970), 127138.Google Scholar
[4]Lovelock, D., ‘Degenerate Lagrange densities involving geometric objects’, Arch. Rational Mech. Anal. 36 (1970), 292304.Google Scholar
[5]Rund, H., ‘Variational problems involving combined tensor fields’, Abh. Math. Sem. Univ. Hamburg 29 (1966), 243262.Google Scholar