This paper discusses self-sustaining oscillations of high-Reynolds-num
ber shear layers and jets incident on edges and corners at infinitesim
al Mach number. These oscillations are frequently sources of narrow-ba
nd sound, and are usually attributed to the formation of discrete vort
ices whose interactions with the edge or corner produce impulsive pres
sures that lead to the formation of new vorticity and complete a feedb
ack cycle of operation. Linearized analyses of these interactions are
presented in which free shear layers are modelled by vortex sheets. De
tailed results are given for shear hows over rectangular wall aperture
s and shallow cavities, and for the classical jet-edge interaction. Th
e operating stages of self-sustained oscillations are identified with
poles in the upper half of the complex frequency plane of a certain im
pulse response function. It is argued that the real parts of these pol
es determine the Strouhal numbers of the operating stages observed exp
erimentally for the real, nonlinear system. The response function coin
cides with the Rayleigh conductivity of the 'window' spanned by the sh
ear flow for wall apertures and jet-edge interactions, and to a freque
ncy dependent drag coefficient for shallow wall cavities. When the int
eraction occurs in the neighbourhood of an acoustic resonator, exempli
fied by the flue organ pipe, the poles are augmented by a sequence of
poles whose real parts are close to the resonance frequencies of the r
esonator, and the resonator can 'speak' at one of these frequencies (b
y extracting energy from the mean flow) provided the corresponding pol
e has positive imaginary part. The Strouhal numbers predicted by this
theory for a shallow wall cavity agree well with data extrapolated to
zero Mach number from measurements in air, and predictions for the jet
-edge interaction are in excellent accord with data from various sourc
es in the literature. In the latter case, the linear theory also agree
s for all operating stages with an empirical, nonlinear model that tak
es account of the formation of discrete vortices in the jet.