Time and Clocks: A Description of Ancient and Modern Methods of Measuring TimeCunynghame, Henry H. (Henry Hardinge), Sir
Philosophy
Time and Clocks: A Description of Ancient and Modern Methods of Measuring Time
Cunynghame, Henry H. (Henry Hardinge), Sir
Clocks and watches; Time
A little consideration will easily show that there are some times
during the swing of a pendulum at which interference is far more
fatal to its time-keeping than at others. Thus the bob of a pendulum
may be regarded as a weight shot outwards from its position of rest
against the influence of a retarding force varying as its distance
from rest—in fact, shot out against a spring. The time of going out
and coming in again will be quite independent of the force exerted to
throw it out, quite independent of its original velocity. Therefore
a variation in the impulse given to the bob is of no consequence,
provided that impulse is given when the bob is near the position of
rest. This follows from the nature of the motion. If a ball be attached
to a piece of elastic thread, and thrown from the hand, so that it
flies out, and then stops and is brought back by the elastic force of
the thread, the time of the outward motion and the return is the same
whatever be the force of the throw. And so if a pendulum be impelled
outwards from a position of rest, the time of the swing out and back
is the same, however big (within limits) is the impelling force and
the consequent length of the swing. The use of a pendulum as a measure
of time is to impel it outwards, and then let it fly _freely_ out and
back. But if its motion is not free, if forces other than gravity act
upon it while on its path, then its time of swing will be disturbed.
It does not matter with what force you originally impel it, but what
does matter is, that when it once starts it should be allowed to travel
unimpeded and uninfluenced. Now that is what an anchor escapement does
not do. The impulse is given the whole way out on one of the pallets,
and then when it is at its extreme of swing, and ought to be left
tranquil, the other pallet fastens on it. But a perfect escapement
ought to give its impulse at the middle point of the swing, when the
pendulum is at the lowest, and then cease, and allow the pendulum to
adapt its swing to the impulse it has received, and thus therefore to
keep its time constant. This is done by an escapement called the dead
beat escapement, which, though in an imperfect way, realises these
conditions.
The alteration is made in the shape of the pallets of the anchor. The
wheel is much the same. Each pallet consists of two faces: a driving
face _a b_ and a sliding face _b c_.
[Illustration]
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