enough to lift off either or all of the legs, and
the plate is gently tapped with the finger, a rattle
is heard, which is the tell-tale of imperfect contact
of all the points. The screw is now reversed
gently and slowly until the moment the rattle
ceases, and then the reading is taken. Here the
sense of hearing is brought into play. This is
also the case when the electric contact is used.
This is so arranged that the instant of touching of
the point of screw, a, completes the electric
circuit, in which an electromagnet of short thick
wire is placed. At the moment of contact, or perhaps
a little before contact, the bell rings, and the turning
of the screw must be instantly stopped. Here
are several elements that must be remembered.
First, it takes time to set the bell ringing, time
for the sound to pass to the ear, time for the sensation
to be carried to the brain, time for the brain to
send word to the hand to cease turning the screw, and,
if you please, it takes time for the hand to stop.
You may say, of what use are such refinements?
I may reply, what use is there in trying to do anything
the very best it can be done? If our investigation
of nature’s profound mysteries can be partially
solved with good instrumental means, what is the result
if we have better ones placed in our hands, and what,
we ask, if the best are given to the physicist?
We have only to compare the telescope of Galileo,
the prism of Newton, the pile of Volta, and what was
done with them, to the marvelous work of the telescope,
spectroscope, and dynamo of to-day. But I must
proceed. It will be recognized that in working
with the spherometer, only the points in actual contact
can be measured at one time, for you may see by Fig.
6 that the four points, a a a a, may all be
normal to a true plane, and yet errors of depression,
as at e, or elevation, as at b, exist
between them, so that the instrument must be used
over every available part of the surface if it is
to be tested rigorously. As to how exact this
method is I cannot say from actual experience, as
in my work I have had recourse to other methods that
I shall describe. I have already quoted you the
words of Prof. Harkness. Dr. Hastings, whose
practical as well as theoretical knowledge is of the
most critical character, tells me that he considers
it quite easy to measure to 1/80000 of an inch with
the ordinary form of instrument. Here is a very
fine spherometer that Dr. Hastings works with from
time to time, and which he calls his standard spherometer.
It is delicately made, its screw being 50 to the inch,
or more exactly 0.01998 inch, or within 2/100000 of
being 1/50 of an inch pitch. The principal screw
has a point which is itself an independent screw,
that was put in to investigate the errors of the main
screw, but it was found that the error of this screw
was not as much as the 0.00001 of an inch. The
head is divided into two hundred parts, and by estimation