There is now sufficient information to attempt an integrated model for melt
generation, transfer and storage beneath subduction-zone volcanoes. Fluid
release from the subducting oceanic crust into the mantle wedge may occur o
ver a period ranging from a few hundred kyr, to as little as less than 1 ky
r, before eruption. This supports models in which fluid addition is closely
linked to partial melting, though there may also be evidence for a compone
nt of decompression melting. The timing of the onset of fluid addition may
be linked to the rate of subduction (i.e. water supply rate) and the angle
of subduction, and, consequently, the thermal structure of the mantle wedge
. In contrast, contributions from subducted sediments to subduction-zone la
va sources appear to occur some 350 kyr-4 Myr before eruption. Evidence for
partial melting of the sediment component, combined with the short fluid t
ransfer times, phenocryst equilibration temperatures and other observations
all point to quite high mantle wedge temperatures close to the interface w
ith the subducting plate. New Ra-226 data permit only a short period of tim
e between fluid addition and eruption. This requires rapid melt segregation
, magma ascent by channelled flow and minimal residence time within the lit
hosphere. Typically, the evolution from basalt to andesite occurs rapidly d
uring ascent or in magma reservoirs, inferred from some geophysical data to
lie within the lithospheric mantle. Mineral isochron data suggest that som
e andesitic magmas subsequently stall in more shallow crustal level magma c
hambers, where they can evolve to dacitic compositions via fractionation, t
ypically combined with assimilation, on time-scales of a few thousand years
or less.