Abstract
It is shown that there is no unique definition of magnetic field line motion with or without perfectly conducting surfaces. Rather, an infinite set of velocity fields exists, each of which can properly be said to describe the motion of magnetic field lines. This set includes, but is not limited to, all possible bounce-averaged motions of charged particles. The supposed discrepancy between the observations of Lezniak and Winckler (1970) and those of Vasyliunas (1968) on plasma sheet motion during substorms is only apparent and illustrates the use of different definitions of field line motion in the same physical situation.
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