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The interaction of charged particles with electromagnetic fields

The interaction of charged particles with electromagnetic fields [Pg.352]

We now turn to the construction of the appropriate perturbation Hamiltonian. To ensure the correct identification of conjugated variables the proper route is [Pg.352]

In 1892 Helmholtz inquired whether we...can cast the empirically known laws of electrodynamics, as they are formulated in Maxwell s equations, in the form of a minimal principle [44]. Indeed such a minimal principle exists in the form of the principle of least action For a system of n degrees of freedom there exists a Lagrangian L qi,qi,t) such that the action integral [Pg.353]

The Lagrangian has the general form L = T — U, where T is the kinetic energy, or more generally the interaction-free part, and U is the generalized potential [Pg.353]

In a conservative system the generalized potential is independent of the velocity q. The extension to continuous systems is done with the introduction of a Lagrangian density [Pg.353]




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Charge of particles

Charged particles

Charged particles interaction

Charging of particles

Electromagnetic field

Interacting field

Interaction electromagnetic

Interaction field

Interaction of particles

Interaction with electromagnetic field

Particle charge

Particle charging

Particle field charging

Particle interaction

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