The semi-solid state of metallic alloys is characterized by the coexistence
of solid and liquid phases at thermal equilibrium. The rheology of such di
phasic materials not only depends on the solid fraction, hut also is highly
correlated with the degree of aggregation of the solid particles. The visc
osity eta of a diphasic (30% and 40% solid fractions) Ag-Cu alloy was measu
red using a contactless method: at 923 degrees C, we get eta = (2 +/- 1) x
10(3) Pa s for a solid fraction of 30% and eta = (2 +/- 1) x 10(4) Pa s for
a solid fraction of 40%. The solid, copper-rich phase, is dispersed into g
lobules of about 50 mu m in size. The large value of eta suggests that thes
e particles form a random interconnected network. This type of microstructu
re is Likely to give rise to the thixotropic rheological properties of many
semi-solid materials. The structure and therefore the viscosity are sensit
ive to the applied shear rate (gamma) over dot. Two distinct regimes of agg
regation, depending on the actual value of the shear rate, are discussed: '
compact clusters' versus 'random network'. We calculate the characteristic
size of the compact clusters and discuss the parameters governing the state
of aggregation.