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Melt in the Mantle
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Melt in the Mantle

Author: Cambridge University

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The Earth's mantle is almost entirely solid, but on geological timescales it convects vigorously, the well-known surface expression of this being plate tectonics. At depths up to ~100 km beneath plate-tectonic boundaries (mid-ocean ridges and subduction zones), and beneath ocean islands such as Hawaii, the mantle melts, and that melt rises to the surface to feed volcanism and form new crust. Such magmatism plays a key role in the chemical evolution and dynamics of our planet. Although the basic thermodynamics of melt generation in these settings is well understood, how the melt is transported to the surface is not, despite several decades of work on the problem. Furthermore, recent observational evidence suggests that mantle melting is not restricted to the near surface (top 100 km): it may occur within the mantle transition zone (410-660 km depth) and above the core-mantle boundary (2900 km). For these deeper instances of melting, an understanding of the dynamical and thermochemical characteristics is currently lacking.

Understanding the formation and migration of melt in the mantle presents a formidable scientific and mathematical challenge. One key challenge is in bridging diverse length scales - melt lies along grain boundaries at micron scales, may focus into channels at metre scales, and migrates over 100 km. Sophisticated mathematical techniques, such as homogenisation theory, are needed to map an understanding of physics at the smallest scales to plate-tectonic scales. Seismology offers a way to image melt in the mantle, but the development of new tools in inverse theory are required to extract that information. Models of melt transport are eventually cast as a series of coupled non-linear partial differential equations, which require advanced numerical techniques to solve. This programme will bring together a broad spectrum of mathematicians and solid Earth scientists to tackle these and other fundamental challenges of melt in the mantle.
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Montesi, L (University of Maryland) Thursday 16th June 2016 - 14:15 to 15:30
Grove, R (Clemson University) Thursday 26th May 2016 - 14:15 to 15:30
Heister, T - Dannberg, J (Texas A&M University) Friday 10th June 2016 - 09:00 to 11:00
Kendall, M (University of Bristol) Friday 10th June 2016 - 11:30 to 12:30
Neufeld, J (University of Cambridge) Friday 10th June 2016 - 14:00 to 14:45
Rees Jones, D (University of Oxford) Thursday 9th June 2016 - 14:45 to 15:30
Showalter, R (Oregon State University) Thursday 9th June 2016 - 16:15 to 17:00
Butler, S (University of Saskatchewan) Thursday 9th June 2016 - 11:30 to 12:30
Schulze, T (University of Tennessee) Thursday 9th June 2016 - 14:00 to 14:45
Arbogast, T (University of Texas at Austin) Wednesday 8th June 2016 - 09:00 to 11:00
Wittum, G (Goethe-Universität Frankfurt) Thursday 9th June 2016 - 09:00 to 11:00
Takei, Y (University of Tokyo) Wednesday 8th June 2016 - 11:30 to 12:30
Karato, S (Yale University) Wednesday 8th June 2016 - 14:45 to 15:30
Yi, S-Y (University of Texas at El Paso) Wednesday 8th June 2016 - 14:00 to 14:45
Rhebergen, S (University of Waterloo) Tuesday 7th June 2016 - 09:00 to 11:00
Suckale

Suckale

2016-06-1448:51

Suckale, J (Stanford University) Tuesday 7th June 2016 - 16:15 to 17:00
Keller, T (University of Oxford) Tuesday 7th June 2016 - 11:30 to 12:30
Kaus, B (Johannes Gutenberg-Universität Mainz, University of Southern California) Tuesday 7th June 2016 - 14:45 to 15:30
Gerya, T (ETH Zürich) Monday 6th June 2016 - 16:15 to 17:00
Wiens, D (Washington University in St. Louis) Monday 6th June 2016 - 11:30 to 12:30
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