Whereas nonrelativistic mechanics always connects the total momentum of a
system to the motion of the center of mass, relativistic systems, such as
interacting electromagnetic charges, can have internal linear momentum in the
absence of motion of the center of energy of the system. This internal linear
momentum of the system is related to the controversial concept of "hidden
momentum." We suggest that the term "hidden momentum" be abandoned. Here we use
the relativistic conservation law for the center of energy to give an
unambiguous definition of the "internal momentum of a system," and then we
exhibit this internal momentum for the system of a magnet (modeled as a
circular ring of moving charges) and a distant static point charge. The
calculations provide clear illustrations of this system for three cases: a) the
moving charges of the magnet are assumed to continue in their unperturbed
motion, b) the moving charges of the magnet are free to accelerate but have no
mutual interactions, and c) the moving charges of the magnet are free to
accelerate and also interact with each other. It is noted that when the
current-carrying charges of the magnet are allowed to interact, the magnet
itself will contain internal electromagnetic linear momentum, something which
has not been presented clearly in the research and teaching literature.Comment: 23 pages. This manuscript is related to arXiv:1408.3741, but has been
thoroughly revised with a different focu