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Electromagnetic and Force Field Equations
Author(s) -
Farahat Sameer Ismail
Publication year - 1994
Publication title -
fortschritte der physik/progress of physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.469
H-Index - 71
eISSN - 1521-3978
pISSN - 0015-8208
DOI - 10.1002/prop.2190420804
Subject(s) - classical mechanics , inhomogeneous electromagnetic wave equation , physics , galilean invariance , maxwell's equations , lorentz covariance , classical field theory , invariant (physics) , electromagnetic field , galilean , dynamical systems theory , lorenz gauge condition , mathematical physics , theory of relativity , gauge theory , lorentz transformation , introduction to gauge theory , quantum mechanics , optical field , gauge anomaly
In classical physics the electromagnetic equations are described by Maxwell's equations. Maxwell's equations proved to be invariant under gauge, or Lorentz transformations. Also, Einstein's equations of the special theory of relativity are invariant under Lorentz transformations. On the other hand classical mechanics and quantum mechanics laws are invariant under Galilean transformations. This means that, there are two different dynamical structures describing our universe. Einstein's unified field theory failled in putting our universe in one dynamical structure. New electromagnetic and force field equations are going to be derived. They have the same shape like Maxwell's equations, but with different dynamical structure. Those equations are invariant under Galilean transformations and in the density matrix formalism of quantum mechanics.