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Introduction to Acoustics

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terms. In this equation γ is the ratio of specific heats and<br />

c 2 o<br />

= γ po<br />

ρo<br />

1<br />

�<br />

1 + ∂ξ<br />

� . (6.71)<br />

γ −1<br />

∂a<br />

One can also generalize this equation in a form which<br />

applies �<strong>to</strong> all � fluids. By expanding the equation of state<br />

γ<br />

ρ<br />

p = po in powers of the condensation s = ρo<br />

ρ−ρo , ρo<br />

one obtains<br />

p = po + As + B<br />

2! s2 + ... and<br />

c 2 = c 2 � � � �<br />

B<br />

o 1 + s + ... . (6.72)<br />

A<br />

This makes it possible <strong>to</strong> obtain the nonlinear wave<br />

equation in the form [6.24]:<br />

∂2ξ =<br />

∂t2 �<br />

1 + ∂ξ<br />

∂a<br />

c2 o<br />

� B<br />

2+ A<br />

∂2ξ . (6.73)<br />

∂a2 In this form one can recognize that the quantity 2 + B/A<br />

for fluids plays the same role as γ + 1 for ideal gases.<br />

Values of B/A for fluids given in Table 6.3 indicate that<br />

nonlinearity of fluids, even in the absence of bubbles of<br />

air, cannot always be ignored. The nonlinearity of fluids<br />

is discussed in greater detail in Chap. 8.<br />

6.5.2 Nonlinearity of Solids<br />

The propagation of a wave in a nonlinear solid is described<br />

by first introducing third-order elastic constants.<br />

When extending the stress–strain relationship (which essentially<br />

is a force-based approach) it becomes difficult<br />

<strong>to</strong> keep a consistent approximation among the various<br />

nonlinear terms. However, If one instead uses an energy<br />

approach, a consistent approximation is au<strong>to</strong>matically<br />

maintained for all the terms of higher order.<br />

Beginning with the elastic potential energy, one can<br />

define both the second-order constants (those determining<br />

the wave velocity in the linear approximation)<br />

and the third-order elastic constants simultaneously. The<br />

Table 6.4 K2 and K3 for the principal directions in a cubic crystal<br />

Direction K2 K3<br />

[100] C11 C111<br />

[110]<br />

[111]<br />

C11 +C12 +2C44 2<br />

C11 +2C12 +4C44 3<br />

Table 6.3 Values of B/A<br />

C 111 +3C 112 +12C 166<br />

4<br />

1<br />

9 (C111 + 6C112 + 12C144 + 24C166 + 2C123 + 16C456)<br />

Physical <strong>Acoustics</strong> 6.5 Nonlinear <strong>Acoustics</strong> 235<br />

Substance T ( ◦ C) B/A<br />

Distilled water 0 4.2<br />

20 5.0<br />

40 5.4<br />

60 5.7<br />

80 6.1<br />

100 6.1<br />

Sea water (3.5%) 20 5.25<br />

Methanol 20 9.6<br />

Ethanol 0 10.4<br />

20 10.5<br />

40 10.6<br />

N-propanol 20 10.7<br />

N-butanol 20 10.7<br />

Ace<strong>to</strong>ne 20 9.2<br />

Beneze 20 9/0<br />

Chlorobenzene 30 9.3<br />

Liquid nitrogen b.p. 6.6<br />

Benzyl alcohol 30 10.2<br />

Diethylamine 30 10.3<br />

Ethylene glycol 30 9.7<br />

Ethyl formate 30 9.8<br />

Heptane 30 10.0<br />

Hexane 30 9.9<br />

Methyl acetate 30 9.7<br />

Mercury 30 7.8<br />

Sodium 110 2.7<br />

Potassium 100 2.9<br />

Tin 240 4.4<br />

Mona<strong>to</strong>mic gas 20 0.67<br />

Dia<strong>to</strong>mic gas 20 0.40<br />

elastic potential energy is<br />

φ (η) = 1 �<br />

2!<br />

ijkl<br />

+ 1<br />

3!<br />

Cijklηijηkl<br />

�<br />

Cijklmnηijηklηmn + ... , (6.74)<br />

ijklmn<br />

Part B 6.5

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