Abstract
Clausius force as equivalent to a time-instant Lorentz force. Action-reaction opposition expressed with the help of potential momenta QA. Conservation of a system's total mass, linear, angular and barycentric momenta. Automatic rendering of the 1967 “hidden momentum in magnets” effect. Clausius formalism asthe low velocity approximation to the Wheeler-Feynman electrodyanmics.
Similar content being viewed by others
References
A. Koch Torres Assis,Weber's Electrodynamics (Kluwer Academic, Dordrecht, 1994), p. 244.
R. Clausius,Ann. Phys. (Leipzig) 135, 606 (1868).
O. Costa de BeauregardPhys. Lett. A 183, 41 (1993).
O. Costa de BeauregardPhys. Lett. A 24, 177 (1967).
P. Penfield and H. Haus,Electrodynamics of Moving Media (M.I.T. Press, Cambridge, Mass., 1967), p. 202 and following.
W. Shockley and R. P. James,Phys. Rev. Lett. 18, 876 (1967).
M. Jouguet,Traité d'Electromagnétisme Théorique, t.3 (Gauthier-Villars, Paris, 1960), p. 126.
W. Weber,Werke (Springer, Berlin, 1893), pp. 25–214.
C. G. Darwin,Phil. Mag. 39, 537 (1920).
S. Coleman and J. H. Van Vleck,Phys. Rev. 171, 1370 (1968).
O. Costa de BeauregardPhys. Lett. A 28, 365 (1968).
J. A. Wheeler and R. P. Feynman,Rev. Mod. Phys. 17, 157 (1945).
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Costa de Beauregard, O. Electrodynamics of interacting point charges: Excellence of the 1865 clausius approximation. Found Phys Lett 9, 151–156 (1996). https://doi.org/10.1007/BF02186257
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF02186257