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A Charged Particle in an Electromagnetic Field

A particle with charge e and mass m moving under the influence of an electromagnetic field experiences the force field [Pg.77]

This can be rewritten using the result from vector analysis that u X (V X A) = V(u A) — (u V)A [Pg.77]

In order to derive an expression for the energy of interaction between an intrinsic magnetic moment (as for a particle with nonzero spin angular momentum) and the electromagnetic field, one cannot proceed via classical mechanics as for the charged particle. Rather one proceeds via the relativistic Dirac equation and seeks the nonrelativistic limit [Pg.78]

The result is that the energy of interaction between the intrinsic magnetic moment jl — pd — P Xx,( y,(7z) of an electron and an electromagnetic field is [Pg.78]

The hamiltonian for an electron with charge e and spin s = S (note that = 1) in an electromagnetic field then takes the form [Pg.78]


The Hamiltonian for a charged particle in an electromagnetic field can be obtained from Hamilton s principle and Lagrange s equations of motion (Section 3.3) ... [Pg.224]

Just by considering equation (4) one may speculate that the NACTs might be similar to the electromagnetic vector potential, S. It is known from classical mechanics that the momentum p of a charged particle in an electromagnetic field changes to p — p + eS - a substitution termed as the minimal principle [1]. Due to the correspondence principle the quantum mechanical minimal principle becomes V—>- V+ i(e/fi)S. However, the NACTs in equation (4), when considering each element separately, do not combine with V (because the... [Pg.106]

The above equation can be changed for a charged particle in an electromagnetic field by explicitly replacing the momentum operator for a free particle with the relativistic momentum for charged particles. Suppose we denote the four components of the relativistic momentum of a charge particle by the Greek letters IT, where these components are explicitly related to the ordinary momentum and the vector and scalar potentials in relativistic units as follows ... [Pg.2472]

A Lagrangian for a collection of charged particles in an electromagnetic field can be written down directly using the polarization fields... [Pg.6]

We shall first find that Lagrangian for a system of charged particles in an electromagnetic field which, through the principle of least action, gives the correct equation of motion. The electric and magnetic fields of the electromagnetic field, d and B, respectively, are related to the scalar and vector potentials, and A, by the equations... [Pg.403]

Charge particles in an electromagnetic field move in a manner so as to produce an opposing induced electromagnetic field consistent with any constraints on the charged particles. This phenomenon is called shielding and also occurs in such areas as waveguides... [Pg.2206]

The Lorentz force F on a particle of charge q in an electromagnetic field is... [Pg.54]

Relativity Physics covers all the material required for a first course in relativity. Beginning with an examination of the paradoxes that arose in applying the principle of relativity to the two great pillars of nineteenth-century physics-classical mechanics and electromagnetism-Dr Turner shows how Einstein resolved these problems in a spectacular and brilliantly intuitive way. The implications of Einstein s postulates are then discussed and the book concludes with a discussion of the charged particle in the electromagnetic field. [Pg.238]

A particle of mass m and charge c moving with a velocity v in an electromagnetic field is subjected to a force... [Pg.108]

The Dirac equation [13, 14] is a relativistically correct version of the Schrodinger formalism, valid for spin-1/2 particles (or antiparticles, as we shall see). One can start by writing the Hamiltonian for a particle of charge — e, momentum p and rest-mass m0 in an electromagnetic field with vector potential A and scalar potential (p as... [Pg.150]

From classical field theory we know that the force on a particle of mass m, charge e, and velocity v which is moving in an electromagnetic field is given by... [Pg.101]

For a charged fluid particle moving in an electromagnetic field, the electromagnetic force per unit volume is... [Pg.102]

The vector product occurs in the force law for a charged particle moving in an electromagnetic field. A particle with charge q moving with velocity v in an electric field E and a magnetic induction field B experiences a Lorentz... [Pg.210]

We now move on to the potential experienced by a moving charge in an electromagnetic field. Potentials are related to the force exerted on a particle. For a particle of charge q and velocity u in an electromagnetic field with electric field strength E and magnetic... [Pg.24]

Physics and chemistry are carried out in laboratory frames using coordinate systems to set up experimental devices. Before discussing quantum mechanical processes let us recall the form of the total Hamiltonian for a set of particles having charges qa and masses ma interacting with an electromagnetic field A. This Hamiltonian is given by ... [Pg.313]


See other pages where A Charged Particle in an Electromagnetic Field is mentioned: [Pg.105]    [Pg.178]    [Pg.77]    [Pg.17]    [Pg.108]    [Pg.105]    [Pg.178]    [Pg.77]    [Pg.17]    [Pg.108]    [Pg.347]    [Pg.105]    [Pg.26]    [Pg.62]    [Pg.4]    [Pg.123]    [Pg.136]    [Pg.224]    [Pg.253]    [Pg.11]    [Pg.379]    [Pg.21]    [Pg.123]    [Pg.37]    [Pg.23]    [Pg.26]    [Pg.238]    [Pg.486]    [Pg.487]    [Pg.128]    [Pg.377]    [Pg.188]    [Pg.75]    [Pg.43]    [Pg.150]    [Pg.61]    [Pg.42]   


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