Ns. Bagdassarov et al., MODELING OF MELT SEGREGATION PROCESSES BY HIGH-TEMPERATURE CENTRIFUGING OF PARTIALLY MOLTEN GRANITES .2. RAYLEIGH-TAYLOR INSTABILITY AND SEDIMENTATION, Geophysical journal international, 127(3), 1996, pp. 627-634
The present experimental study deals with the laboratory modelling of
two different mechanisms of gravitational percolation in partially mel
ted rocks: (1) diapiric percolation of heavy material and (2) the sedi
mentation of heavy particles. These two mechanisms of mass transport i
n partially melted rocks result in different scales of the segregation
process in the melt-crystal matrix. A centrifuge furnace was used to
simulate the percolation of the heavy particle layer through the parti
ally molten granite at temperatures of up to 1000 degrees C. Samples o
f Beauvoir granite (Massif Central, France, grain size 0.16-0.5 mm wit
h an initial degree of partial melting similar to 45 per cent) were us
ed as a matrix. A layer of Pt powder suspended in a melt of the same c
omposition as the partially melted matrix was placed on the top of the
granite sample. After centrifuging for various times (up to 2 x 10(4)
s), X-ray images of samples were obtained and the evolution of the pe
rcolation process of heavy suspension in the partially molten granite
was monitored from the Pt particle distribution. The diapiric or finge
r regime of percolation starts when the growth rate of a Raleigh-Taylo
r instability of the heavy layer is faster than the Stokes sedimentati
on velocity of individual particles in the upper layer. This relations
hip is a complex function of the size and initial concentration of hea
vy particles, as well as the ratio of particle to crystal size, the pe
rmeability of the matrix, and the heterogeneity scale in the partially
melted matrix. At small concentrations (several per cent) and at larg
e concentrations (where close packing of heavy particles results in an
anomalous viscosity increase in the upper heavy layer) Stokes sedimen
tation is dominant in the vertical percolation of the heavy material.
The sinking velocity of the diapir decreases when the size of heavy pa
rticles in it becomes comparable with the size of crystals in the part
ially melted granite. In this situation the vertical sinking of the di
apir is not stable and the horizontal instability of the vertical mass
transport starts to become important. Mass transport via diapiric per
colation results in more efficient crystal-melt segregation of partial
ly melted rocks. The percolation of individual particles provides only
local melt-crystal flow on a scale comparable with the heavy particle
size. The diapiric percolation provides a much larger scale of partia
l melt segregation with a length-scale comparable with the diapir size
.