2014 GSA Annual Meeting in Vancouver, British Columbia (19–22 October 2014)

Paper No. 75-3
Presentation Time: 1:35 PM

MELTING SYSTEMATICS IN MID-OCEAN RIDGE BASALTS:  APPLICATION OF A PLAGIOCLASE-SPINEL MELTING MODEL TO GLOBAL VARIATIONS IN MAJOR ELEMENT CHEMISTRY AND CRUSTAL THICKNESS


BEHN, Mark, Department of Geology and Geophysics, Woods Hole Oceanographic Institution, 360 Woods Hole Road, Mail Stop 22, Woods Hole, MA 02543 and GROVE, Timothy, Earth, Atmospheric, and Planetary Sciences, MIT, Cambridge, MA 02139

We present a new model for anhydrous melting in the spinel and plagioclase stability fields that provides enhanced predictive capabilities for the major element compositional variability found in mid-ocean ridge basalts (MORBs). The model is built on the formulation of Kinzler & Grove [JGR, 1992] and Kinzler [JGR, 1997], but incorporates new experimental data collected since these calibrations [Till et al., JGR, 2012]. The melting model is coupled to geodynamic simulations of mantle flow and mid-ocean ridge temperature structure to investigate global variations in MORB chemistry and crustal thickness as a function of mantle potential temperature, spreading rate, mantle composition, and the pattern(s) of melt migration. While the initiation of melting is controlled by mantle temperature, the cessation of melting is primarily determined by spreading rate, which controls the thickness of the lithospheric lid, and not by the exhaustion of clinopyroxene. Spreading rate has the greatest influence on MORB composition at slow to ultra-slow spreading rates (< 2 cm/yr half rate), where the thermal boundary layer becomes thicker than the oceanic crust. A key aspect of our approach is that we incorporate evidence from both MORB major element compositions and seismically determined crustal thicknesses to constrain global variations in mantle melting parameters. Specifically, we show that to explain the global data set of crustal thickness, and Na8 and Fe8 (Na2O and FeO corrected to 8 wt% MgO, respectively) requires a relatively narrow zone over which melts are pooled to the ridge axis. A small subset of the global data is best modeled as melts of a depleted mantle source composition (e.g., DMM – 2% melt). In all cases, our preferred model transports melt to the ridge axis over relatively short horizontal length scales (~25 km). This implies that although melting occurs over a wide region beneath the ridge axis, up to 20–30% of the total melt volume is not extracted, and will eventually refreeze and refertilize the lithosphere. Finally, we find that the temperature range required to explain the global variations in MORB chemistry and crustal thickness is 1300º to 1450ºC, smaller than that predicted by models that rely solely on compositional evidence.