Numerical experiments are described to ascertain how the steady flow p
ast a circular cylinder loses stability as the Reynolds number is incr
eased. A novel feature of the present study is that the cylinder is co
nfined between parallel planes, allowing a more definitive specificati
on of the flow, both experimentally and computationally, than is possi
ble for the unbounded case. Since the structure of the bifurcation is
unclear from the extant literature, with the experimental and computat
ional evidence not in good agreement, a critical appraisal of both set
s of evidence is presented. A study has been made of the formation of
the steady vortex pair behind the cylinder, and it has been determined
that the first appearance of the vortices is not associated with a bi
furcation of the full dynamical problem but instead it is probably ass
ociated with a bifurcation of a restricted kinematical problem. A set
of numerical experiments has been made in which the steady flow past t
he cylinder was perturbed slightly and the ensuing time-dependent moti
ons were computed. These experiments revealed that, for a given blocka
ge ratio, the perturbation would die away at small Reynolds numbers bu
t that, above a critical Reynolds number, the disturbance would be amp
lified and the flow would eventually settle down to a new state compri
sing a time-periodic motion. Experiments were also carried out to dete
rmine the bifurcation point numerically by considering an eigenvalue p
roblem based on a linearization about the computed steady flow past th
e cylinder. The calculations showed that stability is lost through a s
ymmetry-breaking Hopf bifurcation and that, for a given blockage ratio
, the critical Reynolds number was in very good agreement with that es
timated from the time-dependent computations.