[1] Morse P.M, Ingard K.U.
Theoretical acoustics
. New York: McGraw-Hill, Inc.; 1968:191–195 643.
[2] Chiang H.Y, Huang Y.H. Vibration and sound radiation of an electrostatic speaker based on circular diaphragm.
J Acoust Soc Am
. 2015;137(4):1714–1721.
[3] Mellow T.J, Kärkkäinen L.M. On the sound field of a membrane in free space and an infinite baffle.
J Acoust Soc Am
. 2006;120(5):2460–2477.
[4] Streng J.H. Calculation of the surface pressure on a vibrating circular stretched membrane in free space.
J Acoust Soc Am
. 1987;82(2):679–686.
[5] Streng J.H. Sound radiation from a circular stretched membrane in free space.
J Audio Eng Soc
. 1989;37(3):107–118.
[6] Bouwkamp C.J. Theoretical and numerical treatment of diffraction through a circular aperture.
IEEE Trans Antennas Propag
. 1970;AP18(2):152–176.
[7] Walker P.J. New developments in electrostatic loudspeakers.
J Audio Eng Soc
. 1980;28(11):795–799.
[8] Timoshenko S, Woinowsky-Krieger S.
Theory of plates and shells
. New York: McGraw-Hill; 1959:36–41 79-82, 429-435, 533-559.
[9] Reissner E. On axi-symmetrical vibrations of shallow spherical shells.
Q Appl Math
. 1955;13(3):279–290.
[10] Gradowczyk M.H. Some remarks on the theory of shallow spherical shells.
Ing Arch
. 1963;32:297–303.
[11] Gradshteyn I.S, Ryzhik I.M. In: Jeffrey A, ed.
Table of integrals, series, and products
. 6th ed. New York: Academic Press; 2000.
[12] Mellow T.J, Kärkkäinen L.M. On the sound field of a shallow spherical shell in an infinite baffle.
J Acoust Soc Am
. 2007;121(6):3527–3541.
[13] Suzuki H, Tichy J. Sound radiation from an elastically supported circular plate.
J Acoust Soc Am
. 1979;65(1):106–111.
[14] Rdzanek W. Sound radiation of a vibrating elastically supported circular plate.
J Sound Vib
. 2018;434:92–125.
[15] Harris N, Bank G Available from:. In:
A balanced modal radiator. On the CD ROM: audio engineering society convention papers, 119th convention paper 6595, New York, 7−10 October 2005
. Audio Engineering Society Inc.; 2005 60 East 42nd Street, Room 2520, New York, NY 10165−2520.
