Abstract
ASSOCIATED with the change to SI units, there has been considerable discussion of the roles of the vectors H and D in electromagnetism. Much of the confusion arises from the fact that many people do not appreciate how the macroscopic vectors H and D arise when the macroscopic theory of electromagnetism is developed from a microscopic theory. In a microscopic classical theory, for field points in the space between electrons and atomic nuclei, the microscopic electric intensity e and the microscopic magnetic induction b suffice in Maxwell's equations. If the positions and velocities of every atomic charge and atomic magnetic moment are given, then in principle e and b could be calculated. The force on a point charge q would be given by the Lorentz force expression
where u is the velocity of the test point charge.
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References
Corson, D., and Lorrain, P., Introduction to Electromagnetic Fields and Waves (W. H. Freeman, San Francisco, 1962).
Temperly, H. N. V., Nature, 222, 806 (1969).
Rosser, W. G. V., Phys. Bull., 19, 196 (1968).
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ROSSER, W. Four Macroscopic Vectors of Electromagnetism. Nature 224, 577–579 (1969). https://doi.org/10.1038/224577a0
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DOI: https://doi.org/10.1038/224577a0
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