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
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.