INTRODUCTION.

659. We come now to the most important practical application of the

pendulum. The vibrations being always isochronous, it follows that,

if we count the number of vibrations in a certain time, we shall

ascertain the duration of that time. It is simply the product of the

number of vibrations with the period of a single one. Let us take a

pendulum 39·139 inches long; which will vibrate exactly once a second

in London, and is therefore called a seconds pendulum (See Art. 607).

If I set one of these pendulums vibrating, and contrive mechanism by

which the number of its vibrations shall be recorded, I have a means of

measuring time. This is of course the principle of the common clock:

the pendulum vibrates once a second and the number of vibrations made

from one epoch to another epoch is shown by the hands of the clock.

For example, when the clock tells me that 15 minutes have elapsed, what

it really shows is that the pendulum has made 60 × 15 = 900 vibrations,

each of which has occupied one second.

660. One duty of the clock is therefore to count and record the number

of vibrations, but the wheels and works have another part to discharge,

and that is to sustain the motion of the pendulum. The friction of

the air and the resistance experienced at the point of suspension are

forces tending to bring the pendulum to rest; and to counteract the

effect of these forces, the machine must be continually invigorated

with fresh energy. This supply is communicated by the works of the

clock, which will be sufficiently described presently.

661. When the weight driving the clock is wound up, a store of energy

is communicated which is doled out to the pendulum in a very small

impulse, at every vibration. The clock-weight is just large enough to

be able to counterbalance the retarding forces when the pendulum has

a proper amplitude of vibration. In all machines there is some energy

lost in maintaining the parts in motion in opposition to friction and

other resistances; in clocks this represents the whole amount of the

force, as there is no external work to be performed.

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