Geodesic Equation: Generalizing for Functions F

tom.stoer
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The geodesic equation follows from vanishing variation ##\delta S = 0## with

##S[C] = \int_C ds = \int_a^b dt \sqrt{g_{ab}\,\dot{x}^a\,\dot{x}^b}##

In many cases one uses the energy functional with ##\delta E = 0## instead:

##E[C] = \int_a^b dt \, {g_{ab}\,\dot{x}^a\,\dot{x}^b}##

Can this be generalized for other functions f with ##\delta F = 0## and

##F_f[C] = \int_a^b dt \, f\left(\sqrt{g_{ab}\,\dot{x}^a\,\dot{x}^b}\right)##
 
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If the function f is monotone.
 
That was my idea as well, but I don't see how to generalize the proofs used for S and E. They rely partially on the L2 norm, special case of inner product etc.

Wikipedia writes "The minimizing curves of S ... can be obtained by techniques of calculus of variations ... One introduces the energy functional E ... It is then enough to minimize the functional E, owing to the Cauchy–Schwarz inequality ... with equality if and only if |dγ/dt| is constant"
 
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