“…(2.3) W hen K j a1 (j = 1,2), it was shown by Howe (1991) th a t sca inclusion can be expressed in term s of a distribution of monopole, dipole and quadrupole sources (of nom inally equal im portance) concentrated on th e axis of th e cylinder. If 0 Y , Hl respectively denote th e n et P and S waves inciden inclusion, the corresponding scattered potentials 0 S, Hs are determ ined by the equations,…”