The extension of the Biot-Tolstoy exact time-domain solution to the density
contrast wedge is used to develop an iterative procedure that facilitates
construction of the first-order perturbation of the exterior field with res
pect to distinct wave speed for a point source, which is either smoothly sw
itched on and off within a finite time or is oscillatory for all time. In b
oth cases, this perturbation field is symmetric with respect to the source
and field points and appears as an integral over the wedge involving the is
ovelocity solution for the interior region. The 'geometrical acoustics' com
ponents are simplified for 'rational' wedge angles in the switch-on/off cas
e and estimated in the far field in the oscillatory case to be generated by
a ray passing through the wedge, possibly with internal reflection.