A LUMPED-PARAMETER MODEL FOR THE ACOUSTIC POWER OUTPUT FROM A VIBRATING STRUCTURE

Citation
Jb. Fahnline et Gh. Koopmann, A LUMPED-PARAMETER MODEL FOR THE ACOUSTIC POWER OUTPUT FROM A VIBRATING STRUCTURE, The Journal of the Acoustical Society of America, 100(6), 1996, pp. 3539-3547
Citations number
22
Categorie Soggetti
Acoustics
ISSN journal
00014966
Volume
100
Issue
6
Year of publication
1996
Pages
3539 - 3547
Database
ISI
SICI code
0001-4966(1996)100:6<3539:ALMFTA>2.0.ZU;2-2
Abstract
Previous applications of lumped parameter models to acoustic radiation problems assume that the characteristic dimension of the vibrating st ructure is small in comparison to the acoustic wavelength. In this pap er, the frequency range of the lumped parameter model is extended by d ividing the surface of the structure into elements and characterizing the amplitude of the radiation from each element by its volume velocit y. The model is derived by truncating all but the lowest-order (monopo le) terms of a multipole expansion for the acoustic power output. The multipole expansion differs from those derived previously because it i s based on elemental quantities rather than global quantities. By comp aring the full multipole expansion for the power output to the lumped parameter model, the error in the lumped parameter model as a function of the acoustic and structural wavelengths (k and K) and the size of the largest surface element (L) is determined. This approach is genera l and provides a means of determining bounds on the accuracy of any lu mped parameter model based on elemental quantities. For example, the a nalysis predicts that when the overall volume velocity of a vibrating structure is nonzero, the maximum possible error in the lumped paramet er model is equal to C(kL)(KL), where C is a constant. Likewise, when the overall volume velocity of a vibrating structure is zero, the mode l predicts that the maximum possible error in the lumped parameter mod el is equal to C'(KL)(L/R(12)), where C' is another constant, and R(12 ) is the largest distance between any two points on the structure. The results of the analysis show that it is desirable to formulate acoust ic models in terms of elemental volume velocities, because the power o utput predicted by any such model converges absolutely to the correct solution as the element mesh is refined. (C) 1996 Acoustical Society o f America.