The global linear stability of incompressible, two-dimensional shear f
lows is investigated under the assumptions that far-field pressure fee
dback between distant points in the flow field is negligible and that
the basic flow is only weakly non-parallel, i.e. that its streamwise d
evelopment is slow on the scale of a typical instability wavelength. T
his implies the general study of the temporal evolution of global mode
s, which are time-harmonic solutions of the linear disturbance equatio
ns, subject to homogeneous boundary conditions in all space directions
. Flow domains of both doubly infinite and semi-infinite streamwise ex
tent are considered and complete solutions are obtained within the fra
mework of asymptotically matched WKBJ approximations. In both cases th
e global eigenfrequency is given, to leading order in the WKBJ paramet
er, by the absolute frequency omega(o)(X(t)) at the dominant turning p
oint X(t) of the WKBJ approximation, while its quantization is provide
d by the connection of solutions across X(t). Within the context of th
e present analysis, global modes can therefore only become time-amplif
ied or self-excited if the basic flow contains a region of absolute in
stability.