By Thide B.

ISBN-10: 0470025964

ISBN-13: 9780470025963

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Panofsky and Melba Phillips. Classical Electricity and Magnetism. , Reading, MA . . , third edition, 1962. ISBN 0-201-05702-6. Draft version released 15th January 2000 at 11:38 31 Draft version released 15th January 2000 at 11:38 32 C HAPTER 3 Electromagnetic Potentials Instead of expressing the laws of electrodynamics in terms of electric and magnetic fields, it turns out that it is often more convenient to express the theory in terms of potentials. In this Chapter we will introduce and study the properties of such potentials.

H. Panofsky and Melba Phillips. Classical Electricity and Magnetism. , Reading, MA . . , third edition, 1962. ISBN 0-201-05702-6. [8] Julius Adams Stratton. Electromagnetic Theory. , New York, NY and London, 1953. ISBN 07-062150-0. [9] Jack Vanderlinde. Classical Electromagnetic Theory. , New York, Chichester, Brisbane, Toronto, and Singapore, 1993. ISBN 0-471-57269-1. 1d) can be viewed as an axiomatic basis for classical electrodynamics. In particular, these equations are well suited for calculating the electric and magnetic fields E and B from given, prescribed charge distributions ρ t x and current distributions j t x of arbitrary time- and space-dependent form.

3 The process of choosing a particular gauge condition is referred to as gauge fixing. 14) on page 36 for φ t x and A t x represent a set of uncoupled equations involving four scalar equations (one equation for φ and one equation for each of the three components of A). 19) where Ψ is a shorthand for either φ or one of the vector components of A, and f is the pertinent generic source component. 3. 23) which is a 3D inhomogeneous time-independent wave equation, often called the 3D inhomogeneous Helmholtz equation.

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