“…A more rigorous calculation of the directivity characteristic of an ele mentary area of a transmitter in a solid is presented in [13]. The simplest estimate of the scattered field at the point, r t , for a transmitting element and at the point, r r , for a receiving element can be written in the form (5) where D w, o (α 1, t ) and D o, w (α 1, r ) are the pressure refractive indices for the angles α 1, t and α 1, r for waves passing from the wedge to the TO and back, respectively. The coefficient of reflection from a side hole whose diameter is smaller than the wavelength is assumed to be equal to V(α t , α r , r) = -1, and s(t) is the shape of the received signal.…”