The microrheology of dry soap foams subjected to quasistatic, simple sheari
ng flow is analyzed. Two different monodisperse foams with tetrahedrally cl
ose-packed (TCP) structure are examined: Weaire-Phelan (A15) and Friauf-Lav
es (C15). The elastic-plastic response is evaluated by using the Surface Ev
olver to calculate foam structures that minimize total surface area at each
value of strain. The foam geometry and macroscopic stress are piecewise co
ntinuous functions of strain. The stress scales as T/V-1/3, where T is surf
ace tension and V is cell volume. Each discontinuity corresponds to large c
hanges in foam geometry and topology that restore equilibrium to unstable c
onfigurations that violate Plateau's laws. The instabilities occur when the
length of an edge on a polyhedral foam cell vanishes. The length can tend
to zero smoothly or abruptly with strain. The abrupt case occurs when a sma
ll increase in strain changes the energy profile in the neighborhood of a f
oam structure from a local minimum to a saddle point, which can lead to sym
metry-breaking bifurcations. In general, the new structure associated with
each stable solution branch results from an avalanche of local topology cha
nges called T1 transitions. Each T1 cascade produces different cell neighbo
rs, reduces surface energy, and provides an irreversible, film-level mechan
ism for plastic yield behavior. Stress-strain curves and average stresses a
re evaluated by examining foam orientations that admit strain-periodic beha
vior. For some orientations, the deformation cycle includes Kelvin cells in
stead of the original TCP structure; but the foam does not remain perfectly
ordered. Bifurcations during subsequent T1 cascades lead to disorder and c
an even cause strain localization. (C) 2000 The Society of Rheology. [S0148
-6055(00)00303-5].