able to obtain, the particles are bodily
thrown off and projected to a considerable distance; but with
sufficiently high frequencies no such thing would occur: in such case
only a stress would spread or a vibration would be propagated through
the bulb. It would be out of the question to reach any such frequency
on the assumption that the atoms move with the speed of light; but I
believe that such a thing is impossible; for this an enormous
potential would be required. With potentials which we are able to
obtain, even with a disruptive discharge coil, the speed must be quite
insignificant.

As to the "non-striking vacuum," the point to be noted is that it can
occur only with low frequency impulses, and it is necessitated by the
impossibility of carrying off enough energy with such impulses in high
vacuum since the few atoms which are around the terminal upon coming
in contact with the same are repelled and kept at a distance for a
comparatively long period of time, and not enough work can be
performed to render the effect perceptible to the eye. If the
difference of potential between the terminals is raised, the
dielectric breaks down. But with very high frequency impulses there
is no necessity for such breaking down, since any amount of work can
be performed by continually agitating the atoms in the exhausted
vessel, provided the frequency is high enough. It is easy to
reach--even with frequencies obtained from an alternator as here
used--a stage at which the discharge does not pass between two
electrodes in a narrow tube, each of these being connected to one of
the terminals of the coil, but it is difficult to reach a point at
which a luminous discharge would not occur around each electrode.

A thought which naturally presents itself in connection with high
frequency currents, is to make use of their powerful electro-dynamic
inductive action to produce light effects in a sealed glass globe. The
leading-in wire is one of the defects of the present incandescent
lamp, and if no other improvement were made, that imperfection at
least should be done away with. Following this thought, I have carried
on experiments in various directions, of which some were indicated in
my former paper. I may here mention one or two more lines of
experiment which have been followed up.

Many bulbs were constructed as shown in Fig. 32 and Fig. 33.

In Fig. 32 a wide tube T was sealed to a smaller W-shaped tube U, of
phosphorescent glass. I