ERUPTION ENVIRONMENT AND IMPACT

Subsidence of the Kerguelen Plateau

The subsidence of oceanic plateaus is believed to result from cooling and contraction of the lithospheric plate on which the plateau is constructed (Detrick et al., 1977). Evidence from ODP Legs 119, 120, and 183 clearly demonstrates that large parts of the SKP and CKP that are now submarine were originally subaerial during plateau construction (Coffin, Frey, Wallace, et al., 2000; Mohr et al., this volume). If the SKP had subsided at similar rates as normal oceanic lithosphere, then original maximum elevations would have been on the order of 1 to 2 km above sea level and much of the SKP's ~500,000-km2 area would at one time have been above sea level (Coffin, 1992).

A major source of uncertainty in assessing oceanic plateau subsidence is estimating original depth (e.g., from microfossils) or elevation above sea level at the time of eruption. Wallace (2002) used dissolved volatiles, whose concentrations are pressure dependent, in pillow rim glasses at Site 1140 on the NKP to estimate original eruption depths. The results suggest an eruption depth of 870 ± 80 m. After taking account of the effect of sediment loading on subsidence (Crough, 1983), this leads to an estimated subsidence for the NKP of 1664 m since 34 Ma (Fig. F11). This value is in excellent agreement with the prediction for 34-Ma normal Indian Ocean lithosphere (Detrick et al., 1977). Although subsidence estimates for the CKP and SKP are more uncertain, Wallace (2002) used ages of the oldest marine sediments at existing drill sites to show that most locations subsided by amounts that are consistent with expectations for normal oceanic lithosphere (Fig. F11). This suggests either that the thermal regime typically associated with cooling oceanic lithosphere, despite some embedded continental components, is mainly responsible for the plateau's subsidence behavior, or that the thermal anomaly associated with the Kerguelen plume reset the thermal age of the continental lithosphere embedded in the plateau to near zero. The one site (Site 1139) that appears to have anomalous subsidence (Fig. F11) is located on Skiff Bank, a bathymetric and gravimetric high ~350 km west-southwest of the Kerguelen archipelago (Fig. F1). Volcanic rocks recovered from Site 1139 have been dated at 68-69 Ma (Duncan, 2002), but Skiff Bank appears to be structurally related to the NKP, on which flood basalt eruptions occurred until ~24 Ma (Frey et al., 2000b). Reusch (this volume) uses data for benthic foraminifers to show that Skiff Bank has been at a depth of 1000-2000 m from the early Oligocene to the present. He suggests that Skiff Bank subsided 1-2 km during the first 35 m.y. following emplacement of the volcanic rocks (so that originally subaerial rocks reached a water depth of 1-2 km), but that subsequently their subsidence was minimal. An alternative is that because Skiff Bank is structurally related to the NKP, thermal subsidence of Skiff Bank might have been minimal for several tens of millions of years after its formation, due to dynamic uplift associated with the Kerguelen hotspot, thermal rejuvenation of the lithosphere, or a combination thereof. This model is compatible with the data for benthic foraminifers if Skiff Bank began to subside like normal oceanic lithosphere starting at ~45 Ma (i.e., ~25 m.y. following emplacement).

Volatile Release to the Environment during Formation of the Kerguelen Plateau

The release of volatiles such as CO2, S, Cl, and F accompanying eruption of enormous volumes of basaltic magma during formation of the Kerguelen Plateau and Broken Ridge probably had significant environmental consequences. The role of subaerial volcanic eruptions (Barron, Larsen, et al., 1989; Schlich, Wise, et al., 1989; Coffin, 1992; Coffin, Frey, Wallace, et al., 2000) is significant in this regard because basaltic magmas are nearly completely degassed during subaerial eruptions, whereas hydrostatic pressure inhibits vesiculation and degassing of relatively soluble volatile components (H2O, S, Cl, and F) during deepwater submarine eruptions (Moore, 1970; Moore and Fabbi, 1971; Unni and Schilling, 1978). In contrast to the more soluble magmatic volatiles, the very low solubility of CO2 causes it to be mostly degassed even at abyssal depths (Gerlach, 1989).

Determining the volatile fluxes from Kerguelen Plateau magmatism to the environment is difficult because of relatively poor knowledge about primary magmatic volatile contents, magma volume fluxes through time, and the proportion of volcanic activity that was subaerial or in a shallow submarine environment. Nevertheless, it is possible using existing data to make order of magnitude estimates for volatile release in order to consider potential environmental effects. The magma output rate of the Kerguelen hotspot between 120 and 95 Ma, when the SKP, CKP, and Broken Ridge were formed, was ~1 km3/yr (Coffin et al., 2002) (Fig. F3). The magma output rate appears to have decreased after that time (95 to ~25 Ma) to values of ~0.1 km3/yr. Based on these output rates, the S contents of enriched Site 1140 glasses, and assuming that 50% of the SKP, CKP, and Broken Ridge formed by subaerial eruptions (Coffin, 1992), the estimated S flux to the atmosphere from 120 to 95 Ma would have been 1.4 x 1012 g S/yr (Wallace, 2002). This value is ~13% of the current global flux of S to the atmosphere from subaerial volcanic eruptions (Andres and Kasgnoc, 1998).

An important factor that would have increased the environmental consequences of volcanic S release during formation of the Kerguelen Plateau is the high latitude at which the plateau formed (Frey et al., 2000a). In most basaltic eruptions, released volatiles remain in the troposphere, but at high latitudes, the tropopause is relatively low. As a result, large mass flux basaltic fissure eruption plumes have the potential to transport SO2 and other volatiles into the stratosphere (Stothers et al., 1986; Self et al., 1998). Sulfuric acid aerosol particles that form in the stratosphere after such eruptions have a longer residence time and greater global dispersal than if the SO2 remains in the troposphere, thereby resulting in greater effects on climate and atmospheric chemistry. Although the value of 1.4 x 1012 g S/yr estimated above for the period of Kerguelen Plateau formation from 120 to 95 Ma is only ~13% of the current global flux of S from subaerial volcanic eruptions, it is comparable in magnitude to the estimate of ~0.2 x 1012 to 2 x 1012 g S/yr injected into the stratosphere by explosive eruptions (Pyle et al., 1996).

The magma output rates of Coffin et al. (2002) can also be used to estimate the magnitude of volcanic CO2 release during formation of the SKP, CKP, and Broken Ridge. Assuming a range in primary CO2 contents based on normal MORB, enriched MORB, and ocean-island basalt magmas (~0.2-0.6 wt% CO2) leads to a range of estimates from 0.5 x 1013 to 1.4 x 1013 g CO2/yr released from Kerguelen Plateau volcanism from 120 to 95 Ma. This is ~5% to 10% of the current global annual flux of CO2 released by mid-ocean-ridge and subduction zone volcanism (Gerlach, 1991; Varekamp et al., 1992). Although the magnitude of CO2 release from Kerguelen Plateau volcanism appears to be relatively small compared to the total global volcanic flux, a recent reconstruction of atmospheric CO2 variations during the last 300 m.y. (Retallack, 2001) shows two periods of pronounced CO2 increase that correspond to the times of formation, respectively, of the SKP and CKP. It should be pointed out, however, that the latter period also partially overlaps with formation of both the Caribbean LIP and the Madagascar flood basalt (Coffin and Eldholm, 1994; Eldholm and Coffin, 2000).

Explosive Felsic Volcanism

Highly explosive felsic eruptions, such as those that produced the pyroclastic deposits on Elan Bank, Skiff Bank, and the CKP, can also inject both particulate material and volatiles (SO2 and CO2) directly into the stratosphere (McCormick et al., 1995). The previously unrecognized significant volume of explosive felsic volcanism that occurred when the Kerguelen Plateau and Broken Ridge were subaerial would have further contributed to the effects of this plume volcanism on global climate and environment (Frey et al., 2000a). The total volume of felsic volcanic rocks is poorly constrained, but Leg 183 drilling results indicate that they account for a significant fraction of the volcanic deposits erupted during the final stages of magmatism at several locations on the Kerguelen Plateau.

Analyses of rhyolitic glass inclusions trapped in quartz and sanidine phenocrysts in the tuff at Site 1137 on Elan Bank indicate dissolved magmatic H2O concentrations of 2 to 6 wt% (Wallace et al., 2000). Such concentrations are sufficient to sustain a powerful Plinian eruption column that can reach stratospheric altitudes (Wilson et al., 1980). Although dissolved S contents of the inclusions are relatively low (P.J. Wallace, unpubl. data), the presence of significant CO2 makes it likely that the felsic magmas were vapor saturated before eruption. This is important because the vapor phase may contain significant S (e.g., Scaillet et al., 1998). As a result, eruptions of vapor-saturated silicic magmas typically release large amounts of SO2 derived from the vapor phase, despite the very low concentrations of dissolved S in such magmas (Wallace, 2001).

Environmental Effects of Submarine Hydrothermal Activity

In addition to the potential environmental effects of subaerial volcanism, submarine volcanism and hydrothermal activity during formation of the Kerguelen Plateau and Broken Ridge may also have had important effects on ocean chemistry. Duncan (2002) notes that the seawater Sr isotopic evolution curve exhibits a decline from ~122 to 112 Ma and suggests that this results from large contributions of relatively unradiogenic Sr from hydrothermal activity. Formation of much of the submarine Ontong Java Plateau in the western Pacific at ~122 Ma (Tejada et al., 1996) may also have contributed significantly to seawater Sr changes. However, the importance of hydrothermal activity during formation of oceanic plateaus has not been established. For the Kerguelen Plateau and Broken Ridge a potentially major source of Sr is weathering and erosion of subaerial basalt flows and subsequent riverine transport of Sr to the oceans. Duncan (2002) concludes that if the decrease in seawater radiogenic Sr from 122 to 112 Ma is caused by Kerguelen Plateau hydrothermal activity, then significant submarine volcanism must have ceased between ~115 and ~93 Ma. The latter is the next time period when a sharp decrease in the seawater Sr isotopic evolution curve is seen. Based on new radiometric ages, Duncan (2002) also suggests that rapid submarine construction of the SKP by 118-119 Ma may have contributed to a global environmental crisis recorded by widespread marine black shales (global anoxic event OAE1). Formation of much of the submarine Ontong Java Plateau in the western Pacific at ~122 Ma (Tejada et al., 1996) may also have contributed significantly to this anoxic event.

Subaerial Lava Flow Emplacement Mechanisms and Alteration

A wide variety of mafic subaerial lava types were recovered during Leg 183. A review of the characteristics of these lava types and a refined method for classifying flows recovered in core based on macroscopic textural features is provided by Keszthelyi (this volume). Excluding flow units that cannot be classified because of poor core recovery or intense alteration, Keszthelyi (this volume) concludes that of 30 flow units from Sites 1136, 1137, 1138, and 1139, 7% are slab pahoehoe, 13% are aa, 27% are pahoehoe, and 53% are rubbly pahoehoe. The last of these—rubbly pahoehoe—refers to a lava type that has a flow top composed of broken pieces of smaller pahoehoe lobes. Keszthelyi considers rubbly pahoehoe to be distinct from slab and other recognized types of pahoehoe and suggests that it is a common flow type in Iceland and the Columbia River Basalt Group.

Kurnosov et al. (this volume) show that the subaerial basalts have been variably altered by low-temperature hydrothermal processes (<120°C), and some have been affected by subaerial weathering. Important secondary minerals associated with the hydrothermal alteration include smectites and chlorite minerals. Alteration of the subaerial basalts appears to be related primarily to horizontal fluid flow within permeable contact zones between lava flows (Kurnosov et al., this volume). No soil horizons between basalt flows were recovered at any of the Leg 183 drill sites (Coffin, Frey, Wallace, et al., 2000), but this could be due to the difficulty of recovering thin layers of soft material between basalt during rotary core barrel coring rather than the real absence of soils.

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