[1]
See IEC 60268–5, ed. 3.1. Sound system equipment - part 5: loudspeakers. Available from: http://webstore.iec.ch/. For example, for a nominal 8-in (200 mm) diameter loadspeaker, the baffle size would be 1.65 m long by 1.35 m wide, with the loadspeaker offset from the center by 22.5 cm lengthways and 15 cm widthways.
[2] Small R.H. Closed-box loudspeaker systems Part I: analysis.
J Audio Eng Soc
. 1972;20(10):798–808.
[3] Small R.H. Closed-box loudspeaker systems Part II: synthesis.
J Audio Eng Soc
. 1973;21(1):11–18.
[4] Villchur E.M. Problems of bass reproduction in loudspeakers.
J Audio Eng Soc
. 1957;5(3):122–126.
[5] Backman J.
Improvement of one-dimensional loudspeaker models, in the 123rd AES convention
Paper No. 7253. 2007.
[6] Attenborough K. Acoustical characteristics of porous materials.
Phys Rep
. 1982;82(2):179–227.
[7] Zarek J.H.B. Sound absorption in flexible porous materials.
J Sound Vib
. 1978;61(2):205–234.
[8] Delany M.E, Bazley E.N. Acoustical properties of fibrous absorbent materials.
Appl Acoust
. 1970;3:105–116.
[9] Miki Y. Acoustical properties of porous materials, modification of Delany-Bazley models.
J Acoust Soc Jpn
. 1990;11:19–24.
[10] Sides D.J, Attenborough K, Mulholland K.A. Application of a generalized acoustic propagation theory of fibrous absorbents.
J Sound Vib
. 1971;19:49–64.
[11] Wright J.R. The virtual loudspeaker cabinet.
J Audio Eng Soc
. 2003;51(4):244–247.
[12] Venegas R, Umnova O. Acoustical properties of double porosity granular materials.
J Acoust Soc Am
. 2011;130(5):2765–2776.
[13]
At 1000 Hz, a wavelength at 22°C is about 35 cm; at 500 Hz, 70 cm; at 2000 Hz, 17.5 cm; and so on.
[14] Backman J. Computation of diffraction for loudspeaker enclosures.
J Audio Eng Soc
. 1989;37(5):353–362.
[15] Vanderkooy J. A simple theory of cabinet edge diffraction.
J Audio Eng Soc
. 1991;39(12):923–933.
[16] Svensson U.P. Line integral model of transient radiation from planar pistons in baffles.
Acta Acust Acust
. 2001;87:307–315.
[17] Thuras A.L.
U.S. Patent No. 1,869,178 sound translating device
. July 1932 (filed 1930).
[18] Locanthi B.N. Applications of electric circuit analogies to loudspeaker design problems, IRE trans. Audio, PGA-6: 15 (1952); republished in.
J Audio Eng Soc
. 1971;19(9):778–785.
[19] Novak J.F. Performance of enclosures for high-compliance loudspeakers.
J Audio Eng Soc
. 1959;7(1):29–37.
[20] Thiele A.N. Loudspeakers in vented boxes.
Proc IREE
. 1961;22:487 [republished in J Audio Eng Soc 1971;19(5):382–392 and 1971;19(6):471–83].
[21] Small R.H. Vented-box loudspeaker systems Part I: small-signal analysis.
J Audio Eng Soc
. 1973;21(5):363–372.
[22] Small R.H. Vented-box loudspeaker systems Part II: large-signal analysis.
J Audio Eng Soc
. 1973;21(6):438–444.
[23] Small R.H. Vented-box loudspeaker systems Part III: synthesis.
J Audio Eng Soc
. 1973;21(7):549–554.
[24] Small R.H. Vented-box loudspeaker systems Part IV: appendices.
J Audio Eng Soc
. 1973;21(8):635–639.
[25] Mellow T.J.
A new set of fifth and sixth-order vented-box loudspeaker system alignments using a loudspeaker-enclosure matching filter: Part I, in the 112th AES convention
Paper No. 5505. 2002.
[26] Mellow T.J.
A new set of fifth and sixth-order vented-box loudspeaker system alignments using a loudspeaker-enclosure matching filter: Part II, in the 112th AES convention
Paper No. 5506. 2002.
[27] Thiele A.N. Estimating the loudspeaker response when the vent output is delayed.
J Audio Eng Soc
. 2002;50(3):173–175.
[28] Werner R.E. Effect of negative impedance source on loudspeaker performance.
J Audio Eng Soc
. 1957;29(3):335–340.
[29] Linkwitz S.H. Active crossover networks for noncoincident drivers.
J Audio Eng Soc
. 1976;24(1):2–8.
[30] Linkwitz S.H. Passive crossover networks for noncoincident drivers.
J Audio Eng Soc
. 1978;28(3):149–150.
[31] Bullock III. R.M. Loudspeaker-crossover systems: an optimal crossover choice.
J Audio Eng Soc
. 1982;30(7/8):486–495.
[32] Vanderkooy J, Lipshitz S.P. Power response of loudspeakers with noncoincident drivers – the influence of crossover design.
J Audio Eng Soc
. 1986;34(4):236–244.
[33] Hawksford M.O.J. Asymmetric all-pass crossover alignments.
J Audio Eng Soc
. 1993;41(2):123–134.
[34] Thiele A.N. Passive all-pass crossover system of order 3 (low pass) + 5 (high pass), incorporating driver parameters.
J Audio Eng Soc
. 2002;50(12):1030–1038. .
[35] Thiele A.N. Implementing asymmetrical crossovers.
J Audio Eng Soc
. 2007;55(10):819–832.
[36] Recklinghausen D.R. Low-frequency range extension of loudspeakers.
J Audio Eng Soc
. 1985;33(6):440–446.
[37] Mathes R.C, Miller R.L. Phase effects in monaural perception.
J Acoust Soc Am
. 1947;19(5):780–797.
[38] Craig J.H, Jeffress L.A. Effect of phase on the quality of a two-component tone.
J Acoust Soc Am
. 1962;34(11):1752–1760.
[39] Cabot R.C, Mino M.G, Dorans D.A, Tackel I.S, Breed H.E. Detection. Of phase shifts in harmonically related tones.
J Audio Eng Soc
. 1976;24(7):568–571.
[40] Ashley J.R. Group and phase delay requirements for loudspeaker systems. In:
Proc. IEEE int. conf. on acoustics, speech, and signal processing (Denver, CO, 1980 Apr. 9–11)
. vol. 3. 1980:1030–1033.
[41] Lipshitz S.P, Pocock M, Vanderkooy J. On the audibility of midrange phase distortion in audio systems.
J Audio Eng Soc
. 1982;30(9):580–595.
[42] Schuck P.L. Design of optimized loudspeaker crossover networks using a personal computer.
J Audio Eng Soc
. 1986;34(3):124–142.