It is well known that the existence of edge waves is directly related
to the localization of the acoustic field in the wedge. In this paper,
it is shown experimentally and numerically that, for wedge angles sma
ller than about 100 degrees (this angle may vary from one material to
an other), the edge modes are confined in the tip of the wedge and may
be considered as localized. For higher wedge angles, the analysis of
the results shows a delocalization of the guided waves, which induces
a new repartition of the acoustical energy in the wedge and a decrease
in the amplitude of the wedge wave. This observation is numerically v
erified via an analysis in the time domain. Experiments realized on ob
tuse wedges demonstrate that the first ASF mode may be detected for we
dge angles up to about 110 degrees. (C) 1998 Elsevier Science B.V. All
rights reserved.