Karlisbad
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That's my question..although in more general cases L=T-V
H=T+V however there're several important exceptions..for example:
a) Classically (Non relativisitc) the Gravitational "Energy" (=Hamiltonian for a time-independent Potential) is:
H=(1/2)\int_{V}\rho (\gra \phi)^{2}
b) Einstein-HIlbert Lagrangian L=\sqrt (-g) R -g is the
determinant of the metric and R is Ricci scalar.
Is there always a kind of "transform" so you can always split te Lagrangian into a Kinetic and a potential terms...

H=T+V however there're several important exceptions..for example:
a) Classically (Non relativisitc) the Gravitational "Energy" (=Hamiltonian for a time-independent Potential) is:
H=(1/2)\int_{V}\rho (\gra \phi)^{2}
b) Einstein-HIlbert Lagrangian L=\sqrt (-g) R -g is the
determinant of the metric and R is Ricci scalar.
Is there always a kind of "transform" so you can always split te Lagrangian into a Kinetic and a potential terms...

