The investigation of transonic viscous-inviscid interactions is hampered by
the fact that the nonlinear small disturbance equation which governs the e
xternal flow has to be solved simultaneously with the nonlinear boundary la
yer equations. This poses an extremely difficult numerical problem which ha
s been treated so far with limited success only. However, if the medium is
confined in a sufficiently narrow channel, the pow outside the viscous wall
layers is one-dimensional in the leading order approximation which in turn
allows the derivation of a solution in closed form. This significantly sim
plifies the construction of numerical solutions which nevertheless display
essential features of transonic flows associated with the transition from s
ubsonic to supersonic conditions or/and vice versa.