A mechanical vibration is the motion of a particle or a body which
oscillates about a position of equilibrium. Most vibrations in machines
and structures are undesirable because of the increased stresses and
energy losses which accompany them. They should therefore be eliminated
or reduced as much as possible by appropriate design. The
analysis of vibrations has become increasingly important in recent
years owing to the current trend toward higher-speed machines and
lighter structures. There is every reason to expect that this trend will
continue and that an even greater need for vibration analysis will develop
in the future.
The analysis of vibrations is a very extensive subject to which entire
texts have been devoted. Our present study will therefore be limited
to the simpler types of vibrations, namely, the vibrations of a body
or a system of bodies with one degree of freedom.
A mechanical vibration generally results when a system is displaced
from a position of stable equilibrium. The system tends to return
to this position under the action of restoring forces (either elastic
forces, as in the case of a mass attached to a spring, or gravitational
forces, as in the case of a pendulum). But the system generally reaches
its original position with a certain acquired velocity which carries it
beyond that position. Since the process can be repeated indefinitely,
the system keeps moving back and forth across its position of equilibrium.
The time interval required for the system to complete a full
cycle of motion is called the period of the vibration. The number of
cycles per unit time defines the frequency, and the maximum displacement
of the system from its position of equilibrium is called the
amplitude of the vibration.
When the motion is maintained by the restoring forces only, the
vibration is said to be a free vibration (Secs. 19.2 to 19.6). When a
periodic force is applied to the system, the resulting motion is described
as a forced vibration (Sec. 19.7). When the effects of friction
can be neglected, the vibrations are said to be undamped. However,
all vibrations are actually damped to some degree. If a free vibration
is only slightly damped, its amplitude slowly decreases until, after a
certain time, the motion comes to a stop. But if damping is large
enough to prevent any true vibration, the system then slowly regains
its original position (Sec. 19.8). A damped forced vibration is maintained
as long as the periodic force which produces the vibration is
applied. The amplitude of the vibration, however, is affected by the
magnitude of the damping forces (Sec. 19.9).
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