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The Hamiltonian of a system is defined as
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(1) |
where q is a generalized coordinate, p is a generalized momentum, L is the Lagrangian, and
Einstein summation has been used. If L is a sum of functions homogeneous (i.e., no products of different
degrees) in generalized velocities of degrees 0, 1, and 2 and the equations defining the generalized coordinates are not
functions of time, then
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(2) |
where T is the kinetic energy, V is the potential energy, and E is the total energy of the system.
Hamiltonian Mechanics, Hamiltonian Operator, Kamiltonian
© 1996-2007 Eric W. Weisstein
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