T1-5
1.5 Principles of Noise Reduction
A good vibration isolation system is reducing vibration transmission through structures and thus, radiation of these
vibration into air, thereby reducing noise.
There are many ways to reduce noise. One of the most practical and effective may be the use of vibration mounts. As a
general rule, a well-designed vibration isolator will also help reduce noise. In the case of panel flutter, for example, a well-
designed vibration mount could reduce or eliminate the noise. This can be achieved by eliminating the flutter of the panel
itself, or by preventing its transmission to ground, or by a combination of the two. The range of audible frequencies is so high
that the natural frequencies of a vibration mount can usually be designed to be well below the noise-producing frequency.
In order to reduce noise, try to identify its sources; e.g., transformer hum, panel flutter, gear tooth engagement, rotor
unbalance, etc. Next, identify the noise frequencies. Vibration isolators for these sources designed in accordance with the
guidelines for vibration and shock control may then act as barriers either in not conducting the sound, or in attenuating the
vibration which is the source of the noise.
2.0 BASIC DEFINITIONS AND CONCEPTS IN VIBRATION AND SHOCK ANALYSIS
2.1 Kinematic Characteristics
COORDINATE A quantity, such as a length or an angle, which defines the position of a moving part. In Figure 1, x is
a coordinate, which defines the position of the weight, W.
DISPLACEMENT A change in position. It is a vector measured relative to a specified position, or frame of reference.
The change in x (Figure 1) measured upward, say, from the bottom position, is a displacement. A displacement can be
positive or negative, depending on the sign convention, translational or rotational. For example, an upward displacement
may be positive, and a downward displacement negative. Similarly, a clockwise rotation may be positive and a counterclock-
wise rotation negative. Units: inches, feet, meters (m), millimeters (mm), or, in the case of rotations: degrees, radians, etc.
VELOCITY The rate of change of displacement. Units: in/sec, mph., m/sec, etc. Velocity is a vector whose magnitude
is the SPEED. Angular velocity might be measured in radians/sec or deg/sec, clockwise or counterclockwise.
ACCELERATION The rate of change of velocity. Units: in/sec2, m/sec2, etc. It is a vector and has a magnitude and
direction. Angular acceleration might be measured in rad/sec2 or deg/sec2, clockwise or counterclockwise.
VIBRATORY MOTION An oscillating motion; such as, that of the weight W, in Figure 1.
SIMPLE VIBRATORY MOTION A form of vibratory motion, which as a function of the time is of the form x = a sin 3t,
where a and 3 are constants. The maximum displacement, a, from the mean position (x = 0) is the AMPLITUDE; the
FREQUENCY (rate at which the motion repeats itself) is f = 3/23 cycles/sec, where ANGULAR FREQUENCY 3 has the
dimensions of rad/sec, and frequency f has the dimensions of reciprocal time; e.g. reciprocal seconds 1/sec. Such motion is
also called harmonic or sinusoidal motion.
PERIOD, CYCLE The interval of time within which the motion repeats itself. In Figure 5, this is T seconds. The term
cycle tends to refer also to the sequence of events within one period.
AMPLITUDE Figure 5 shows time history of a vibratory motion, which repeats itself every T seconds. The maximum
values of the displacement, x, from the reference position (x = 0) are called PEAKS. These are (a1, a2...). The largest of these
is called the PEAK AMPLITUDE.
STEADY-STATE MOTION A periodic motion of a mechanical system; e.g., a continuously swinging pendulum of
constant amplitude.
STOCHASTIC or RANDOM MOTION A motion which changes with time in a nonperiodic, possibly very complex,
manner.
Figure 5 Periodic Motion
0
x
T
2T
3T
Time, t, secs
a1
a2
a5
a6
a3
a4