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Hamiltonian
(redirected from Hamiltonians)

   Also found in: Wikipedia 0.01 sec.
Ham·il·to·ni·an  (hml-tn-n)
n. Abbr. H
A mathematical function that can be used to generate the equations of motion of a dynamic system, equal for many such systems to the sum of the kinetic and potential energies of the system expressed in terms of the system's coordinates and momenta treated as independent variables.

[After Sir William Rowan Hamilton (1805-1865), Irish mathematician.]

Hamiltonian [ˌhæməlˈtəʊnɪən] Physics Maths
n
1. (Physics / General Physics) a mathematical function of the coordinates and momenta of a system of particles used to express their equations of motion
2. (Physics / General Physics) a mathematical operator that generates such a function. Symbol H
adj
(Physics / General Physics) denoting or relating to the Irish mathematician Sir William Rowan Hamilton (1805-65), or to the theory of mechanics or mathematical operator devised by him

Hamiltonian  (hml-tn-n)
A mathematical function or operator that can be used to describe the state of a physical system. In classical mechanics, the Hamiltonian is a function of coordinates and momenta of bodies in the system, treated as independent variables. It is equal to the sum of the kinetic and potential energies of the system, and can be used to derive the equations of motion for the system. In quantum mechanics, the Hamiltonian is an operator corresponding to the total energy of the system. The Hamiltonian is named after Irish mathematician William Rowan Hamilton (1805-1865).


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For those with a deep interest in understanding such things, this book provides a reasonably accessible, technically precise and thorough account of all of math's major aspects--from the basics of algebra, geometry, algorithms and proofs to the essential features of Hilbert spaces and Hamiltonians.
Hamiltonians were out in great numbers to show their sadness and their appreciation of our emergency services.
Jurdjevic covers Cartan decomposition and the generalized elastic problems, the maximum principle and the Hamiltonians, the left-invariant symplectic form, symmetries and the conservation laws, complex Lie groups and complex Hamiltons, complexified elastic problems, complex elasticae of Euler and its n-dimensional extensions, Cartan algebras, root spaces and extra integrals of motion, and elastic curves in the cases of Lagrange and Kowalewski.
 
 
 
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