Stokes' law (sound attenuation)

Stokes derived law for attenuation of sound in Newtonian liquid [ Stokes, G.G. "On the theories of the internal friction in fluids in motion, and of the equilibrium and motion of elastic solids", "Transaction of the Cambridge Philosophical Society", vol.8, 22, pp. 287-342 (1845] . According to this law attenuation of sound α is proportional to the dynamic viscosity η, square of the sound frequency ω, and reciprocally proportional to the liquid density ρ and cubic power of sound speed V

:$alpha\; =\; frac\{2\; etaomega^2\}\{3\; ho\; V^3\}$

Attenuation is expressed in neper per meter in this equation. The author of this law is the same famous Stokes who derived well known Stokes' law for the friction force in fluids. It is 160 years old. This remarkable law does not contain unknown or un-measurable parameters.

:It is convenient to convert attenuation into other units, by normalizing attenuation with respect to frequency, because the attenuation typically increases rapidly with frequency. These new units make more adequate presentation of attenuation within a wide frequency range.It is seen that attenuation of the Newtonian liquid, presented in these units, becomes a linear function of frequency.

There has been substantial theoretical development in this field since Stokes’ pioneering work. It has brought one important correction to the Stokes law. It turns out that in addition to the dynamic viscosity the parameter of volume viscosity η^v also affects the total attenuation according to the following relationship:

:$alpha\; =\; frac\{2\; (eta+eta^v)omega^2\}\{3\; ho\; V^3\}$

The parameter volume viscosity is surprisingly little known despite its fundamental role for fluid dynamics at high frequencies. This parameter appears in Navier-Stokes equation if it is written for compressible fluid, as described in the most books on general hydrodynamics [ Happel, J. and Brenner , H. "Low Reynolds number hydrodynamics", "Prentice-Hall", (1965)] , [ Landau, L.D. and Lifshitz, E.M. "Fluid mechanics", "Pergamon Press",(1959)] , and the acoustics [ Morse, P.M. and Ingard, K.U. "Theoretical Acoustics", "Princeton University Press"(1986)] , [ Dukhin, A.S. and Goetz, P.J. "Ultrasound for characterizing colloids", "Elsevier", (2002) ] .

This "volume viscosity" coefficient becomes important only for such effects where fluid compressibility is essential and, importantly, ultrasound propagation is one such effect. Indeed, many rheological texts just assume the fluid to be incompressible and the volume viscosity therefore plays no role.

The only values for the volume viscosity of simple Newtonian liquids known to us come from the old Litovitz and Davis review [ Litovitz, T.A. and Davis, C.M. In "Physical Acoustics", Ed. W.P.Mason, vol. 2, chapter 5, "Academic Press", NY, (1964)] . They report a "volume viscosity" of water at 15 C^o equals 3.09 centipoise

:More recent studies have established that Stokes's law is actually a low frequency asymptotic of the more general relationship that describes sound attenuation at very high frequencies:

:$2(frac\{alpha\; V\}\{omega\})^2\; =\; frac\{1\}\{sqrt\{1+omega^2\; au^2\; -frac\{1\}\{1+omega^2\; au^2\}$

where relaxation time τ equals:

:$au\; =\; frac\{1\}\{\; ho\; V^3\}(4\; eta/3\; +\; eta^v)$

Corresponding relaxation frequency is about 1000 GHz. It is extremely high. For all practical purposes of describing sound attenuation in Newtonian liquids Stokes' law is clearly sufficient.

References

External links

* [http://www.dispersion.com/ Dispersion Technology]

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