| Literature DB >> 28514440 |
Rupert Sutherland1,2, John Townend2, Virginia Toy3, Phaedra Upton1, Jamie Coussens4, Michael Allen5, Laura-May Baratin2, Nicolas Barth6, Leeza Becroft3, Carolin Boese2, Austin Boles7, Carolyn Boulton5, Neil G R Broderick8, Lucie Janku-Capova2, Brett M Carpenter9, Bernard Célérier10, Calum Chamberlain2, Alan Cooper3, Ashley Coutts8, Simon Cox11, Lisa Craw3, Mai-Linh Doan12, Jennifer Eccles8, Dan Faulkner5, Jason Grieve3, Julia Grochowski2, Anton Gulley8, Arthur Hartog13, Jamie Howarth1, Katrina Jacobs2, Tamara Jeppson14, Naoki Kato15, Steven Keys2, Martina Kirilova3, Yusuke Kometani16, Rob Langridge1, Weiren Lin17,18, Timothy Little2, Adrienn Lukacs3, Deirdre Mallyon19, Elisabetta Mariani5, Cécile Massiot1,2, Loren Mathewson3, Ben Melosh20, Catriona Menzies4, Jo Moore21, Luiz Morales22, Chance Morgan9, Hiroshi Mori23, Andre Niemeijer24, Osamu Nishikawa25, David Prior3, Katrina Sauer3, Martha Savage2, Anja Schleicher7,26, Douglas R Schmitt19, Norio Shigematsu27, Sam Taylor-Offord2, Damon Teagle4, Harold Tobin14, Robert Valdez28, Konrad Weaver2, Thomas Wiersberg26, Jack Williams3, Nick Woodman4, Martin Zimmer26.
Abstract
Temperature and fluid pressure conditions control rock deformation and mineralization on geological faults, and hence the distribution of earthquakes. Typical intraplate continental crust has hydrostatic fluid pressure and a near-surface thermal gradient of 31 ± 15 degrees Celsius per kilometre. At temperatures above 300-450 degrees Celsius, usually found at depths greater than 10-15 kilometres, the intra-crystalline plasticity of quartz and feldspar relieves stress by aseismic creep and earthquakes are infrequent. Hydrothermal conditions control the stability of mineral phases and hence frictional-mechanical processes associated with earthquake rupture cycles, but there are few temperature and fluid pressure data from active plate-bounding faults. Here we report results from a borehole drilled into the upper part of the Alpine Fault, which is late in its cycle of stress accumulation and expected to rupture in a magnitude 8 earthquake in the coming decades. The borehole (depth 893 metres) revealed a pore fluid pressure gradient exceeding 9 ± 1 per cent above hydrostatic levels and an average geothermal gradient of 125 ± 55 degrees Celsius per kilometre within the hanging wall of the fault. These extreme hydrothermal conditions result from rapid fault movement, which transports rock and heat from depth, and topographically driven fluid movement that concentrates heat into valleys. Shear heating may occur within the fault but is not required to explain our observations. Our data and models show that highly anomalous fluid pressure and temperature gradients in the upper part of the seismogenic zone can be created by positive feedbacks between processes of fault slip, rock fracturing and alteration, and landscape development at plate-bounding faults.Entities:
Year: 2017 PMID: 28514440 DOI: 10.1038/nature22355
Source DB: PubMed Journal: Nature ISSN: 0028-0836 Impact factor: 49.962