The use of a modal representation for the exterior acoustic field of a stru
cture has received increasing attention in recent years. This modal approac
h generally seeks a set of orthogonal functions, representing independent s
urface velocity distributions, termed acoustic radiation modes, which diago
nalize a radiation operator in the exterior domain of the structure. These
orthogonal acoustic radiation modes may be found, among other methods, thro
ugh an eigenvalue analysis of a radiation operator and possess a correspond
ing set of eigenvalues that are proportional to the radiation efficiencies
of the acoustic radiation modes. In free space, the acoustic radiation mode
s of a sphere display a grouping characteristic in their radiation efficien
cies, where each acoustic radiation mode's radiation efficiency within a gr
oup has the same frequency dependency. This is a consequence of the fact th
at the acoustic radiation modes of a sphere al-e the spherical harmonics. F
urther, the acoustic radiation modes of an arbitrary three-dimensional stru
cture exhibit the same frequency grouping as those for the sphere. The basi
s for the arbitrary structure's grouping follows from the sphere's grouping
. The observation that the acoustic radiation modes of an arbitrary body ar
e dominated by spherical harmonics provides insight on the behavior of such
modes. These results have significance for various applications of acousti
c radiation modes, including active noise control design, radiation modelin
g, etc. (C) 2001 Acoustical Society of America. [DOI: 10.1121/1.1323236].