Geochemical observations of MORE including U-series disequilibria are used
to examine the processes and timescales of MORE melt generation. Incompatib
le elements in MORE suggest that the MORE source region consists of a deple
ted Iherzolite matrix interspersed with chemically enriched mafic veins. Wi
de variations in Th/U distinguish these source variations in MORE better th
an Sr-87/Sr-86 and document that the relative chemical homogeneity of norma
l MORE reflects efficient melt mixing rather than a homogeneous source. Spi
nel compositional variations in MORE and in mantle solids (abyssal peridoti
tes and dunites) reflect reactive flow of melts having significant composit
ional variations. High Cr# spinels result from reactive flow of chemically
enriched melts derived from the mafic vein source ascending through the Ihe
rzolite of the upper melting column. High Cr# and TiO2 contents in dunite s
pinels indicate that dunites form by reactive flow of enriched melts throug
h the upper melting column. Once formed, dunites act as high permeability p
athways for melt from surrounding lherzolite and are responsible for the "f
ractional signatures" observed in the major element chemistry, melt inclusi
ons, abyssal peridotites and Lu-Hf systematics of MORE. Based on the recogn
ition that there are two sources melting beneath ridges that have different
porosity characteristics, a melting model consistent with evidence for bot
h fractional and equilibrium porous flow melting is proposed. In this model
, the presence of dunite channels affect melt generation and transport in t
he Iherzolite matrix, suggesting that mantle heterogeneity may be critical
to the physical aspects of melting and melt transport in the mantle beneath
mid-ocean ridges. U-series disequilibria provide information on how meltin
g occurs in the two endmember sources and suggest that melt porosities in t
he Iherzolite may be as low as 0.1%. Melt within Iherzolite maintains equil
ibrium with the coexisting solid while it ascends porously. Primitive MORE
with high Mg# consistently have low Th-230 excesses or deficits with major
element chemical signatures of equilibration near 1.0 GPa suggesting that t
he depleted endmember melt maintains chemical equilibrium with Iherzolite u
ntil shallow mantle depths (similar to 30 km). Melt porosities in enriched
heterogeneities remain below 1% for perhaps 10s of km before losing chemica
l equilibrium with the solid during transport in the upper melting column.
Because the porosities required by the observed disequilibria are small, th
e transition to porosities large enough to form "veins" of melt must occur
over a timescale which is very long in comparison to the Ra-226 half-life a
nd significantly long for Pa-231. Thus, instantaneous transport dynamic mel
ting models appear incompatible with the observed disequilibria even when i
nitial melt productivities as low as 0.05%/km are used. (C) 2000 Elsevier S
cience B.V. All rights reserved.