When the electrified particle is moved
a mass of ether has to be moved too, and thus the apparent mass of the
particle is increased. The mass of the electrified particle is thus
resident in every part of space reached by its lines of force; in this
sense an electrified body may be said to extend to an infinite distance;
the amount of the mass of the ether attached to the particle diminishes
so rapidly as we recede from it that the contributions of regions remote
from the particle are quite insignificant, and in the case of a
particle as small as a corpuscle not one millionth part of its mass will
be farther away from it than the radius of an atom.
The increase in the mass of a particle due to given charges varies as we
have seen inversely as the radius of the particle; thus the smaller the
particle the greater the increase in the mass. For bodies of appreciable
size or even for those as small as ordinary atoms the effect of any
realizable electric charge is quite insignificant, on the other hand for
the smallest bodies known, the corpuscle, there is evidence that the
whole of the mass is due to the electric charge. This result has been
deduced by the help of an extremely interesting property of the mass due
to a charge of electricity, which is that this mass is not constant but
varies with the velocity. This comes about in the following way. When
the charged particle, which for simplicity we shall suppose to be
spherical, is at rest or moving very slowly the lines of electric force
are distributed uniformly around it in all directions; when the sphere
moves, however, magnetic forces are produced in the region around it,
while these, in consequence of electro-magnetic induction in a moving
magnetic field, give rise to electric forces which displace the tubes of
electric force in such a way as to make them set themselves so as to be
more at right angles to the direction in which they are moving than they
were before. Thus if the charged sphere were moving along the line AB,
the tubes of force would, when the sphere was in motion, tend to leave
the region near AB and crowd towards a plane through the centre of the
sphere and at right angles to AB, where they would be moving more nearly
at right angles to themselves. This crowding of the lines of force
increases, however, the potential energy of the electric field, and
since the mass of the ether carried along by the lines of force is
proportional to the potential energy, the mass of the charged particle
will also be increased. The amount of variation of the mass with the
velocity depends to some extent on the assumptions we make as to the
shape of the corpuscle and the way in which it is electrified. The
simplest expression connecting the mass with the velocity is that when
the velocity is v the mass is equal to (2/3)[mu]e²/a [1/(1 - v²/c²)^½]
where c is the velocity of light. We see from this that the variation of
mass with velocity is very small unless the velocity of the body
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