Rv. Craster, A CANONICAL PROBLEM FOR FLUID-SOLID INTERFACIAL WAVE COUPLING, Proceedings - Royal Society. Mathematical, physical and engineering sciences, 452(1950), 1996, pp. 1695-1711
Wave-coupling involving defects or obstacles on fluid-solid interfaces
is of recurrent interest in geophysics, transducer devices, structura
l acoustics, the acoustic microscope and related problems in non-destr
uctive testing. Most theoretical analysis to date has, in effect, invo
lved stress or pressure loadings along the interface, or scattering fr
om surface inhomogeneities, that ultimately result in unmixed boundary
value problems. A more complicated situation occurs if a displacement
is prescribed over a region of the interface, and the rest of the int
erface is unloaded (or stress/pressure loaded); the resulting boundary
value problem is mixed. This occurs if a rigid strip lies along part
of the interface and will introduce several complications due to the p
resence of the edge. For simplicity a lubricated rigid strip is consid
ered, i.e. it is smoothly bonded to the elastic substrate. To consider
such mixed problems, e.g. the vibration of a finite rigid strip or di
ffraction by a finite strip, a canonical semi-infinite problem must be
solved. It is the aim of this paper to solve the canonical problem as
sociated with the vibrating strip exactly, and extract the form of the
near strip edge stress, and displacement fields, and the far-field di
rectivities associated with the radiated waves. The near strip edge re
sults are checked using an invariant integral based upon a pseudo-ener
gy momentum tensor and gives a useful independent check upon this piec
e of the analysis. The directivities will be useful in formulating a r
ay theory approach to finite strip problems. An asymptotic analysis of
the solution, in the far field, is performed using a steepest descent
s approach and the far-field directivities are found explicitly. In th
e light fluid limit a transition analysis is required to determine uni
form asymptotic solutions in an intermediate region over which the lea
ky Rayleigh wave will have an influence. In a similar manner to relate
d work on the acoustic behaviour of fluid-loaded membranes and plates,
there is beam formation in this intermediate region along critical ra
ys.