Time and Clocks: A Description of Ancient and Modern Methods of Measuring Time — John Shaqi
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 reflection will soon convince us that it has none. For we know
that the time that bodies take to fall to the ground under the action
of gravity is independent of the weight. A falling 2 lb. weight is only
equivalent to two pound-weights falling side by side.
In the same way and by the same reasoning we might take two pendulums
of equal length, and each with a bob weighing 1 lb. They would, if put
side by side close together swing in equal times. But the time would be
the same if they were fastened together, and made into one pendulum.
For inasmuch as the fall of a pendulum is due to gravity, and the
action of gravity upon a body is proportional to its mass, it follows
that in a pendulum the part of the gravitational force that acts upon
each part of the mass is occupied in moving that mass, and the whole
pendulum may be considered as a bundle of pendulums tied together and
vibrating together.
The same would be the case with a pendulum vibrating under the
influence of a spring. If you have two bobs and two springs, they will
vibrate in the same time as one bob accelerated by one spring. In
this case, however, the force of the one spring must be equal to the
combined force of the two springs. In other words, the springs must be
made proportional in strength to the masses.
Hence, then, you cannot increase the speed of the vibration of a
pendulum by adding weight to the bob.
On the other hand, if you have a bob vibrating under the influence of a
spring, like the balance wheel of a watch, then if you increase the bob
without increasing the spring, since the mass to be moved has increased
without a corresponding increase in the accelerating force acting on
it, the time of swing will alter accordingly.
But in the case of gravity, by altering the mass, you thereby
proportionally alter the attraction on it, and therefore the time of
swing is unaltered.
[Illustration: FIG. 39.]
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