signals which start and end at zero level and last a finite and relatively short amount of time. They are characterized by a certain amount of “energy” they contain in the same way that continuous signals are characterized by a “power” value. Examples of transient signals are the sound of a car door closing, a shock wave generated by an impact, the noise produced by a sheet metal stamping press, and the noise of an electric spark.

Nonstationary continuous signals are signals consisting of one or more of the following: sinusoidal components with variable amplitudes and/or frequencies, random signals with statistical properties which change with time, and transients which appear with varying intervals and with varying characteristics in time and frequency. Examples of nonstationary continuous signals are the acceleration on the chassis or frame of a truck driving on a rough road, the wind speed for wind‐induced vibrations, the vibrations or chatter induced in machine tools during machining, the vibration produced by a jackhammer, and speech.

1.3 Frequency Analysis

      In noise and vibration control, signal analysis means determining from a measurement or a set of measurements certain descriptive characteristics of the environment that will help in identifying the sources of the noise and vibration. Frequency analysis is probably the most widely used method for studying noise and vibration problems. The frequency content of a noise or vibration signal is usually related to a specific component of a given system, such as a machine, so that frequency analysis is often the key to obtain a better understanding of the causes or sources of the noise and vibration.

      1.3.1 Fourier Series

Sometimes in acoustics and vibration we encounter signals which are pure tones (or very nearly so), e.g. the 120 Hz hum from an electric motor. In the case of a pure tone, the time history of the signal is simple harmonic and could be represented by the waveform x(t) = A sin (2πf₁ t) in Figure 1.2a. The pure tone can be represented in the frequency domain by a spike of height A at frequency f₁, Hz (see Figure 1.2a).

Figure 1.2 Time and frequency domain representations of (a) pure tone; (b) complex tone; and (c) nonperiodic deterministic signal.

      More often, sound signals are encountered which are periodic, but not simple harmonic. These are known as complex tones. Such sound signals are produced by most musical instruments (both wind and string). They can also be produced mechanically or electronically (a square wave is an example of a periodic signal or complex tone). The broken line plotted in Figure 1.2b is an example of a complex tone which is made up by the superposition (addition) of two simple harmonic signals, x(t) = A sin (2πf₁ t) + B sin (2πf₃ t). Note in this case we have chosen f₃ = 3f₁. The signal A sin (2πf₁ t) is known as the fundamental (or first harmonic) and B sin (2πf₃ t) is the third harmonic. In this particular case the second harmonic and the fourth and higher harmonics are completely absent from the complex tone x(t). The frequency domain representation of the complex tone is also given in Figure 1.2b.

      In fact, Fourier [11] showed in 1822 that any periodic signal may be analyzed as a combination of sinusoids:

(1.1)

      or in complex notation:

(1.2)

      where ω = 2πf; f is the fundamental frequency; T = 1/f = 2π/ω, is the period of the signal; j = , and A_n and B_n are the Fourier coefficients calculated from [4, 6, 8]

(1.3a)

(1.3b)

The sine and cosine terms in Eq. (1.1) can have values of the subscript n equal to 1, 2, 3, …, ∞. Hence, the signal x(t) will be made up of a fundamental frequency ω and multiples, 2, 3, 4, …, ∞ times greater. The A₀/2 term represents the D.C. (direct current) component (if present). The nth term of the Fourier series is called the nth harmonic of x(t). The amplitude of the nth harmonic is

(1.4)

      and its square, , is sometimes called energy of the nth harmonic. Thus, the graph of the sequence is called the energy spectrum of x(t) and shows the amplitudes of the harmonics.

      Example 1.1

Buzz‐saw noise is commonly generated by supersonic fans in modern turbofan aircraft engines. A buzzing sound can be represented by the periodic signal shown in Figure 1.3. Find the Fourier series and the energy spectrum for this signal.

      Solution

We are required to represent x(t) = At over the interval 0 ≤ t ≤ 1, T = 1, and the fundamental frequency is ω = 2π/T = 2π. Then, we determine the corresponding Fourier coefficients using Eqs. (1.3a) and (1.3b)

      Therefore, substituting for the Fourier coefficients in Eq. (1.1) we get

The