
NSF Org: |
OCE Division Of Ocean Sciences |
Recipient: |
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Initial Amendment Date: | June 25, 2015 |
Latest Amendment Date: | August 4, 2020 |
Award Number: | 1459387 |
Award Instrument: | Standard Grant |
Program Manager: |
Deborah K. Smith
OCE Division Of Ocean Sciences GEO Directorate for Geosciences |
Start Date: | June 15, 2015 |
End Date: | May 31, 2021 (Estimated) |
Total Intended Award Amount: | $275,137.00 |
Total Awarded Amount to Date: | $315,394.00 |
Funds Obligated to Date: |
FY 2020 = $40,257.00 |
History of Investigator: |
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Recipient Sponsored Research Office: |
8622 DISCOVERY WAY # 116 LA JOLLA CA US 92093-1500 (858)534-1293 |
Sponsor Congressional District: |
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Primary Place of Performance: |
CA US 92093-0244 |
Primary Place of
Performance Congressional District: |
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Unique Entity Identifier (UEI): |
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Parent UEI: |
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NSF Program(s): | Marine Geology and Geophysics |
Primary Program Source: |
01002021DB NSF RESEARCH & RELATED ACTIVIT |
Program Reference Code(s): |
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Program Element Code(s): |
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Award Agency Code: | 4900 |
Fund Agency Code: | 4900 |
Assistance Listing Number(s): | 47.050 |
ABSTRACT
Ocean crust, which makes up about 65% of the volume of Earth's surface, is created at mid-ocean ridges, one of the most dynamic geological environments on the planet. Vast quantities of heat are dissipated along these features, facilitating the generation of large, potentially economic, mineral deposits and hydrothermal vents that host unique chemosynthetic ecosystems that live without the need for sunlight. At mid-ocean ridges, melts from the upwelling mantle rise toward the surface and either erupt as lavas on the seafloor or freeze on their way up, resulting in ocean crust that has a thick coarsely crystalline base made of gabbroic and peridotitic rock covered by a veneer of basaltic lava. With the exception of the surface lavas, the lower portions of crust can only be sampled and studied from deep rips and tears in the seafloor caused by structural features or tectonic processes. One of the places where the gabbroic layer is exposed is a place called the Pito Deep in the eastern Pacific Ocean. This research involves a major multidisciplinary oceanographic expedition to the Pito Deep to both sample and study the lower crustal gabbros of fast spread ocean crust and their relation to overlying basalts and underlying crustal components. On the expedition, samples will also be taken to determine the ancient thermal structure at the ridge axis. Broader impacts of the work include support of an institution and faculty in an EPSCoR state (Wyoming); good student training at the college, community college, and K-12 level; and the inclusion of a K-12 teacher on the cruise to produce educational materials for K-12 and communicate with students back on land.
The science being done in this project has the potential to resolve long standing debates about how gabbroic lower crust is accreted at fast spread mid-ocean ridges and will shed light on unresolved questions regarding the depth of hydrothermal circulation in the seafloor, the width and temporal evolution of the axial magma chamber of mid-ocean ridges, and the processes of melt transport and crystallization between the mantle and the seafloor. Samples will be collected using a remotely operated vehicle, with sampling taking place along a ~20-km long flow line at Pito Deep. The nearly ridge-perpendicular exposures at Pito Deep span multiple geomagnetic polarity intervals, providing a unique opportunity to document the shape of the fossil 580°C isotherm in the lower crust and thus to differentiate between the different thermal predictions of lower crustal accretion models. These end-member models also make predictions of the variation of geochemical, petrologic and microstructural parameters with depth. Major and trace element geochemistry combined with petrofabrics from electron backscattered diffraction will be examined for a significant vertical portion (>1km) of the upper gabbroic layer to further discriminate between these accretion models. While no single crustal exposure is likely to definitively resolve the processes by which the gabbroic lower crust is accreted, the exposures at Pito Deep offer the possibility of addressing outstanding questions regarding the depth of hydrothermal heat extraction, the width and temporal evolution of the axial magma chamber, and the processes of melt transport and crystallization.
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PROJECT OUTCOMES REPORT
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This Project Outcomes Report for the General Public is displayed verbatim as submitted by the Principal Investigator (PI) for this award. Any opinions, findings, and conclusions or recommendations expressed in this Report are those of the PI and do not necessarily reflect the views of the National Science Foundation; NSF has not approved or endorsed its content.
The formation of ocean crust at mid-ocean ridges is one of the fundamental processes of plate tectonics and Earth evolution. While the lava flows comprising the upper ocean crust can be sampled by a variety of methods, deeper portions of the crust that are emplaced and cool more slowly are more difficult to sample, particularly for seafloor generated at the fastest spreading ridges. This slow cooling produces coarse-grained (gabbroic) rocks that constitute about three quarters of the ocean crust formed at fast-spreading ridges, yet because of their relative inaccessibility, their formation remains poorly understood. For example, key aspects of how melt is delivered to the spreading ridge, where it crystallizes or how heat is extracted from the lower crust as it interacts with seawater all remain unclear. This project was designed to address how the lower, gabbroic crust is formed at fast-spreading ridges through study of one of only two locations (Pito Deep in the eastern Pacific) where such rocks are known to be exposed.
Faulting at Pito Deep has exposed an intact crustal sequence including the uppermost gabbros, which preserve a unique record of Earth's magnetic field variations that allowed us to examine the formation and cooling history of the lower crust. As new seafloor lavas erupt and cool they record the Earth's magnetic field direction (Fig. 1). Variations in the direction of the field, either parallel to its present orientation (red) or in the opposite direction (blue), yield a distinctive barcode-like pattern of seafloor magnetic stripes. These directional (polarity) changes are also recorded in the more slowly cooled gabbroic crust, and the three-dimensional pattern of the magnetic stripes at depth preserves a record of the temperature in the lower crust at the time of the reversal. Measurements of the magnetic field near the seafloor allowed us to determine the polarity pattern in the lower crust and a suite of ~230 oriented gabbro samples provided direct confirmation of this pattern. These data reveal a nearly horizontal polarity boundary in the lower crust, extending for a minimum of about 8 km away from the spreading center which indicates that the lower crust remains too hot to acquire a magnetization for about the first 100,000 years after it forms (Fig. 1b). About a third of our samples preserve a record of slow cooling spanning more than one polarity interval. These samples yield additional information on the rate of cooling in the lower crust, which we find ranges from about 0.5 to 2?C per thousand years. The implications of these data are significant as they are incompatible with deep seawater penetration and heat extraction near the ridge axis (Fig. 1a). Instead, our results suggest a broader, warm region near the ridge than in many previous models of construction of fast-spread ocean crust. The companion study of the petrology of the rocks, conducted by collaborators at the University of Wyoming, yields consistent results. More than 300, mostly oriented, samples record hitherto unrecognized petrological and structural complexity, that is best explained by repeated injection of pulses of magma to the top of the gabbroic crust at Pito Deep, followed by crystallization and rotational flow of the resulting crystal mush. This flow can only happen if the uppermost crust cools slowly and remains near solidus temperatures for a significant time.
Last Modified: 12/14/2021
Modified by: Jeffrey S Gee
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