[1] Rayleigh J.W.S. 2nd ed.
Theory of sound
. vol. 2. New York: Dover, Inc; 1945:323–328.
[2] Crandall I.B.
Vibrating systems and sound
. New York: D. Van Nostrand Company, Inc; 1926.
[3] Ingard U. Scattering and absorption by acoustic resonators, doctoral dissertation, Massachusetts Institute of Technology.
J Acoust Soc Am 1953
. 1950;25:1044–1045.
[4] Li X. End correction model for the transfer impedance of microperforated panels using viscothermal wave theory.
J Acoust Soc Am
. 2017;141(3):1426–1436.
[5] Borwick J, ed.
Loudspeaker and headphone handbook
. 3rd ed. Oxford: Focal; 2001:588 Fig. 14.2.
[6] Olson H.F.
Elements of acoustical engineering
. 2nd ed. New York: D. Van Nostrand Company, Inc; 1947:109–111.
[7] Fincham L, Brown P. Line arrays with controllable directional characteristics - theory and practice. In:
The 125th AES convention
. 2008 paper no. 7535.
[8] Walker P.J. New Developments in Electrostatic loudspeakers.
J Audio Eng Soc
. 1980;28(11):795–799.
[9]
See the definition for intensity in Section 1.10. The intensity equals the sound pressure squared, divided by ρ0c for a plane wave in free space or for a spherical wave.
[10] Kozlov V.F, Fedorov A.V. Acoustic properties of rarefied gases inside pores of simple geometries.
J Acoust Soc Am
. 2005;117(6):3402–3412.
[11] Stinson M.R. The propagation of plane sound waves in narrow and wide circular tubes, and generalization to uniform tubes of arbitrary cross-sectional shape.
J Acoust Soc Am
. 1991;89(2):550–558.
[12] Morse P.M, Ingard K.U.
Theoretical acoustics
. New York: McGraw-Hill, Inc; 1968:279 Eq. (6.4.17), p. 281; Eq. (6.4.21), p. 286; Eq. (6.4.31), p. 240; Eq. (6.1.13).
[13] Veijola T. A two-port model for wave propagation along a long circular microchannel.
Microfluid Nanofluidics
. 2007;3(3):359–368.
