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-------··CU<br />

~ ..19· ~~<br />

.0 '\<br />

! Spores Growth \<br />

Fig. 7.4. Formation of colony by the<br />

amoebae Dictyostelium discoidem<br />

.. '\l+;/ spores which are separating<br />

Yr·"<br />

~ Plasmodium ----.. 17. +'- from it into the medium. When<br />

~.. Cell they encounter a nutrient rich<br />

~ . agregation environment, they form a new<br />

colony by way of chemotactic<br />

M::;iO:/ migration (fig. 7.4).<br />

7.3. ACOUSTIC WAVES<br />

7.3.1. Classification of Acoustic Waves<br />

A longitudinal wave that consists of a sequence of pressure<br />

pulses or an elastic displacement of the material, whether gas,<br />

liquid, or solid, is called an acoustic wave. There are three<br />

categories of acoustic waves that cover different ranges of<br />

frequency - sound, ultrasound, and infrasound waves.<br />

7.3.2. Physical Characteristics of Sound Waves<br />

Sound has three physical quannties: frequency (Q), intensity<br />

(I), and waveform which correspond to the characteristics of<br />

sound that we hear - pitch, loudness, and tone quality. Sound<br />

waves that lie within the range of sensitivity of the human ear are<br />

called audible sound waves; these waves have a frequency ranging<br />

between approximately 20 Hz to 20000 Hz.<br />

The pitch of a note is determined by the frequency; the more<br />

vibrations per second of the sound, the higher will be the pitch<br />

of the note.<br />

The intensity or loudness of a sound is a measure of the energy<br />

impinging on a unit area of receiver surface per unit of time. The<br />

units of intensity are therefore W/m 2 • The intensity of the faintest<br />

sound which can just be heard is about 10- 12 W/m2; the loudest<br />

66<br />

tolerable sound has an intensity of approximately 1 W1m 2 •<br />

Because of this wide range in intensities over which the ear operates,<br />

and because the ear can only discriminate between sounds<br />

of a certain intensity ratio whether they are loud or soft, a logarithmic<br />

rather than a linear intensity scale is used. The intensity<br />

level (B) of a sound wave is defined by the equation:<br />

I<br />

B = 19­<br />

1 0<br />

(7.15)<br />

where 1 0<br />

is an arbitrary reference intensity and is conventionally<br />

taken as the threshold for hearing (i.e., 10- 12 W1m 2 ) . The intensity<br />

7.1. Typical values ofthe sound level is a dimensionless<br />

. levels from various sources quantity and the unit is<br />

or causing specific symptoms the bel (B) or more<br />

commonly, the decibel<br />

Source of Sound ] Sound Level,dBJ (dB).<br />

Damage of eardrum 160<br />

Nearby jet airplane<br />

Threshold of pain<br />

Rock concert<br />

Subway<br />

150<br />

130<br />

120<br />

100<br />

I<br />

dB=10Ig­<br />

1 0<br />

Table 7.1 gives<br />

(7.16)<br />

some<br />

Busy traffic 80 typical values for the<br />

Vacuum cleaner 70 sound levels from various<br />

Normal conversation 50 sources or causing spe­<br />

Mosquito buzzling 40 cific symptoms in hu­<br />

Rustling leaves 10 mans.<br />

Example. The intensity of an ultrasound pulse produced by a bat<br />

during echolocation is about 10- 2 W1m 2 • Express this in decibels.<br />

Solution. Using Equation (7.16), we shall find:<br />

I 10- 2<br />

dB = 10 Ig/ = 10 Ig 10- 12<br />

= 10,10 = 100 dB<br />

o<br />

Tone quality corresponds to the complexity of the frequency<br />

composition of the sound produced by the source. A precision<br />

tuning fork will vibrate with only one frequency, producing a pure<br />

tone. However, most vibrating bodies, in addition to the fundamental<br />

or lowest frequency, have harmonics which are frequencies<br />

that are single multi plies of the fundamentals. If f is the<br />

fundamental frequency, then 2f is calIed the second harmonic. The<br />

67

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