Abstract

The Euler-Lagrange equations corresponding to a Lagrange density which is a function of a symmetric affine connection, Γ i j h , and its first derivatives together with a symmetric tensor gi j, are investigated. In general, by variation of the Γ i j h , these equations will be of second order in Γ i j h . Necessary and sufficient conditions for these Euler-Lagrange equations to be of order one and zero in Γ i j h are obtained. It is shown that if the gi j may be regarded as independent then the only permissible zero order Euler-Lagrange equations are those which ensure that the Γ i j h are precisely the Christoffel symbols of the second kind.

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