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Chapter 13: Mid-Ocean Rifts The Mid-Ocean Ridge System Figure 13-1. After Minster et al. (1974) Geophys. J. Roy. Astr. Soc., 36, 541-576. Ridge Segments and Spreading Rates Table 13-1. Spreading Rates of Some Mid-Ocean Ridge Segments • Slow-spreading ridges: < 3 cm/a • Fast-spreading ridges: > 4 cm/a are considered • Temporal variations are also known Category Ridge Fast East Pacific Rise Slow Indian Ocean Mid-Atlantic Ridge Latitude 21-23oN 13oN 11oN 8-9oN 2 oN 20-21oS 33oS 54oS 56oS SW SE Central 85oN 45oN 36oN 23oN 48oS Rate (cm/a)* 3 5.3 5.6 6 6.3 8 5.5 4 4.6 1 3-3.7 0.9 0.6 1-3 2.2 1.3 1.8 From Wilson (1989). Data from Hekinian (1982), Sclater et al . (1976), Jackson and Reid (1983). *half spreading Oceanic Crust and Upper Mantle Structure 4 layers distinguished via seismic velocities Deep Sea Drilling Program Dredging of fracture zone scarps Ophiolites Oceanic Crust and Upper Mantle Structure Typical Ophiolite Figure 13-3. Lithology and thickness of a typical ophiolite sequence, based on the Samial Ophiolite in Oman. After Boudier and Nicolas (1985) Earth Planet. Sci. Lett., 76, 84-92. Oceanic Crust and Upper Mantle Structure Layer 1 A thin layer of pelagic sediment Figure 13-4. Modified after Brown and Mussett (1993) The Inaccessible Earth: An Integrated View of Its Structure and Composition. Chapman & Hall. London. Oceanic Crust and Upper Mantle Structure Layer 2 is basaltic Subdivided into two sub-layers Layer 2A & B = pillow basalts Layer 2C = vertical sheeted dikes Figure 13-4. Modified after Brown and Mussett (1993) The Inaccessible Earth: An Integrated View of Its Structure and Composition. Chapman & Hall. London. Layer 3 more complex and controversial Believed to be mostly gabbros, crystallized from a shallow axial magma chamber (feeds the dikes and basalts) Layer 3A = upper isotropic and lower, somewhat foliated (“transitional”) gabbros Layer 3B is more layered, & may exhibit cumulate textures Oceanic Crust and Upper Mantle Structure Discontinuous diorite and tonalite (“plagiogranite”) bodies = late differentiated liquids Figure 13-3. Lithology and thickness of a typical ophiolite sequence, based on the Samial Ophiolite in Oman. After Boudier and Nicolas (1985) Earth Planet. Sci. Lett., 76, 84-92. Layer 4 = ultramafic rocks Ophiolites: base of 3B grades into layered cumulate wehrlite & gabbro Wehrlite intruded into layered gabbros Below cumulate dunite with harzburgite xenoliths Below this is a tectonite harzburgite and dunite (unmelted residuum of the original mantle) Petrography and Major Element Chemistry A “typical” MORB is an olivine tholeiite with low K2O (< 0.2%) and low TiO2 (< 2.0%) Only glass is certain to represent liquid compositions The common crystallization sequence is: olivine ( Mg-Cr spinel), olivine + plagioclase ( Mg-Cr spinel), olivine + plagioclase + clinopyroxene Figure 7-2. After Bowen (1915), A. J. Sci., and Morse (1994), Basalts and Phase Diagrams. Krieger Publishers. Fe-Ti oxides are restricted to the groundmass, and thus form late in the MORB sequence Figure 8-2. AFM diagram for Crater Lake volcanics, Oregon Cascades. Data compiled by Rick Conrey (personal communication). The major element chemistry of MORBs Originally considered to be extremely uniform, interpreted as a simple petrogenesis More extensive sampling has shown that they display a (restricted) range of compositions Table 13-2. Average Analyses and CIPW Norms of MORBs (BVTP Table 1.2.5.2) The major element chemistry of MORBs Oxide (wt%) SiO2 TiO2 Al2O3 FeO* MgO CaO Na2O K2O P2O5 Total All 50.5 1.56 15.3 10.5 7.47 11.5 2.62 0.16 0.13 99.74 MAR 50.7 1.49 15.6 9.85 7.69 11.4 2.66 0.17 0.12 99.68 EPR 50.2 1.77 14.9 11.3 7.10 11.4 2.66 0.16 0.14 99.63 IOR 50.9 1.19 15.2 10.3 7.69 11.8 2.32 0.14 0.10 99.64 Norm q or ab an di hy ol mt il ap 0.94 0.95 22.17 29.44 21.62 17.19 0.0 4.44 2.96 0.30 0.76 1.0 22.51 30.13 20.84 17.32 0.0 4.34 2.83 0.28 0.93 0.95 22.51 28.14 22.5 16.53 0.0 4.74 3.36 0.32 1.60 0.83 19.64 30.53 22.38 18.62 0.0 3.90 2.26 0.23 All: Ave of glasses from Atlantic, Pacific and Indian Ocean ridges. MAR: Ave. of MAR glasses. EPR: Ave. of EPR glasses. IOR: Ave. of Indian Ocean ridge glasses. MgO and FeO Al2O3 and CaO SiO2 Na2O, K2O, TiO2, P2O5 Figure 13-5. “Fenner-type” variation diagrams for basaltic glasses from the Afar region of the MAR. Note different ordinate scales. From Stakes et al. (1984) J. Geophys. Res., 89, 6995-7028. Conclusions about MORBs, and the processes beneath mid-ocean ridges MORBs are not the completely uniform magmas that they were once considered to be They show chemical trends consistent with fractional crystallization of olivine, plagioclase, and perhaps clinopyroxene MORBs cannot be primary magmas, but are derivative magmas resulting from fractional crystallization (~ 60%) Fast ridge segments (EPR) a broader range of compositions and a larger proportion of evolved liquids (magmas erupted slightly off the axis of ridges are more evolved than those at the axis itself) Figure 13-8. Histograms of over 1600 glass compositions from slow and fast midocean ridges. After Sinton and Detrick (1992) J. Geophys. Res., 97, 197-216. For constant Mg# considerable variation is still apparent. Figure 13-9. Data from Schilling et al. (1983) Amer. J. Sci., 283, 510-586. Incompatible-rich and incompatible-poor mantle source regions for MORB magmas N-MORB (normal MORB) taps the depleted upper mantle source Mg# > 65: K2O < 0.10 TiO2 < 1.0 E-MORB (enriched MORB, also called P-MORB for plume) taps the (deeper) fertile mantle Mg# > 65: K2O > 0.10 TiO2 > 1.0 Trace Element and Isotope Chemistry REE diagram for MORBs Figure 13-10. Data from Schilling et al. (1983) Amer. J. Sci., 283, 510-586. E-MORBs (squares) enriched over N-MORBs (red triangles): regardless of Mg# Lack of distinct break suggests three MORB types E-MORBs La/Sm > 1.8 N-MORBs La/Sm < 0.7 T-MORBs (transitional) intermediate values Figure 13-11. Data from Schilling et al. (1983) Amer. J. Sci., 283, 510-586. N-MORBs: 87Sr/86Sr < 0.7035 and 143Nd/144Nd > 0.5030, depleted mantle source E-MORBs extend to more enriched values stronger support distinct mantle reservoirs for Ntype and E-type MORBs Figure 13-12. Data from Ito et al. (1987) Chemical Geology, 62, 157-176; and LeRoex et al. (1983) J. Petrol., 24, 267-318. Conclusions: MORBs have > 1 source region The mantle beneath the ocean basins is not homogeneous N-MORBs tap an upper, depleted mantle E-MORBs tap a deeper enriched source T-MORBs = mixing of N- and E- magmas during ascent and/or in shallow chambers Experimental data: parent was multiply saturated with olivine, cpx, and opx P range = 0.8 - 1.2 GPa (25-35 km) Figure 13-10. Data from Schilling et al. (1983) Amer. J. Sci., 283, 510-586. Implications of shallow P range from major element data: MORB magmas = product of partial melting of mantle lherzolite in a rising solid diapir Melting must take place over a range of pressures The pressure of multiple saturation represents the point at which the melt was last in equilibrium with the solid mantle phases Trace element and isotopic characteristics of the melt reflect the equilibrium distribution of those elements between the melt and the source reservoir (deeper for E-MORB) The major element (and hence mineralogical) character is controlled by the equilibrium maintained between the melt and the residual mantle phases during its rise until the melt separates as a system with its own distinct character (shallow) MORB Petrogenesis Generation Separation of the plates Upward motion of mantle material into extended zone Decompression partial melting associated with near-adiabatic rise N-MORB melting initiated ~ 60-80 km depth in upper depleted mantle where it inherits depleted trace element and isotopic char. Figure 13-13. After Zindler et al. (1984) Earth Planet. Sci. Lett., 70, 175-195. and Wilson (1989) Igneous Petrogenesis, Kluwer. Generation Region of melting Melt blobs separate at about 25-35 km Figure 13-13. After Zindler et al. (1984) Earth Planet. Sci. Lett., 70, 175-195. and Wilson (1989) Igneous Petrogenesis, Kluwer. Lower enriched mantle reservoir may also be drawn upward and an E-MORB plume initiated Figure 13-13. After Zindler et al. (1984) Earth Planet. Sci. Lett., 70, 175-195. and Wilson (1989) Igneous Petrogenesis, Kluwer. The Axial Magma Chamber Original Model Semi-permanent Fractional crystallization derivative MORB magmas Periodic reinjection of fresh, primitive MORB from below Dikes upward through the extending and faulting roof Figure 13-14. From Byran and Moore (1977) Geol. Soc. Amer. Bull., 88, 556-570. Crystallization near top and along the sides successive layers of gabbro (layer 3) Dense olivine and pyroxene crystals ultramafic cumulates (layer 4) Layering in lower gabbros (layer 3B) from density currents flowing down the sloping walls and floor? Figure 13-14. From Byran and Moore (1977) Geol. Soc. Amer. Bull., 88, 556-570. A modern concept of the axial magma chamber beneath a fastspreading ridge Figure 13-15. After Perfit et al. (1994) Geology, 22, 375-379. The crystal mush zone contains perhaps 30% melt and constitutes an excellent boundary layer for the in situ crystallization process proposed by Langmuir Figure 11-12 From Winter (2001) An Introduction to Igneous and Metamorphic Petrology. Prentice Hall Melt body continuous reflector up to several kilometers along the ridge crest, with gaps at fracture zones, devals and OSCs Large-scale chemical variations indicate poor mixing along axis, and/or intermittent liquid magma lenses, each fed by a source conduit Figure 13-16 After Sinton and Detrick (1992) J. Geophys. Res., 97, 197-216. Model for magma chamber beneath a slow-spreading ridge, such as the Mid-Atlantic Ridge Dike-like mush zone and a smaller transition zone beneath well-developed rift valley Most of body well below the liquidus temperature, so convection and mixing is far less likely than at fast ridges Depth (km) 2 Rift Valley 4 6 Moho Figure 13-16 After Sinton and Detrick (1992) J. Geophys. Res., 97, 197-216. Transition zone Gabbro Mush 8 10 5 0 Distance (km) 5 10 Nisbit and Fowler (1978) suggested that numerous, small, ephemeral magma bodies occur at slow ridges (“infinite leek”) Slow ridges are generally less differentiated than fast ridges No continuous liquid lenses, so magmas entering the axial area are more likely to erupt directly to the surface (hence more primitive), with some mixing of mush Depth (km) 2 Rift Valley 4 6 Moho Transition zone Gabbro Mush 8 10 5 0 Distance (km) 5 Figure 13-16 After Sinton and Detrick (1992) J. Geophys. Res., 97, 197-216. 10 Figures I don’t use in class Figure 13-6. From Stakes et al. (1984) J. Geophys. Res., 89, 6995-7028. Figures I don’t use in class Figure 13-7. Data from Schilling et al. (1983) Amer. J. Sci., 283, 510-586.