Basal Shear Stress of the Ross Ice Streams from Control Method Inversions Ian Joughin Jet Propulsion Lab, California Institute of Technology Slawek Tulaczyk.

Slides:



Advertisements
Similar presentations
Louisiana Tech University Ruston, LA Slide 1 Energy Balance Steven A. Jones BIEN 501 Wednesday, April 18, 2008.
Advertisements

Bed Coupling 1. Introduction 2. Sources of the idea  Boulton's experiments  Remote sensing 3. Processes  sources of strength  the Coulomb equation.
Scaling of viscous shear zones with depth dependent viscosity and power law stress strain-rate dependence James Moore and Barry Parsons.
3-D Finite Element Modeling of the Rise and Fall of the Himalayan-Tibetan Plateau Mian Liu and Youqing Yang Dept. of Geological Sciences, University of.
D.F. Martin 1, S.L. Cornford 2, S.F. Price 5, X. Asay-Davis 3,4, P.O.Schwartz 1, E.G. Ng 1, A.J. Payne 1 Fully-Resolved.
Subglacial conditions of inland West Antarctica from US-ITASE deep radar reflection analysis WAIS Workshop September 30, 2005 Brian Welch, Bob Jacobel.
WAIS 2005; Slide number 1. Numerical modelling of ocean- ice interactions under Pine Island Bay’s ice shelf Tony Payne 1 Paul Holland 2,3 Adrian Jenkins.
Metal Forming Metal forming includes a large group of manufacturing processes in which plastic deformation is used to change the shape of metal work pieces.
Inverting for ice crystal orientation fabric Kristin Poinar Inverse theory term project presentation December 7, 2007 The University of Washington.
California State University, Chico
CE1501 CE 150 Fluid Mechanics G.A. Kallio Dept. of Mechanical Engineering, Mechatronic Engineering & Manufacturing Technology California State University,
Exploring Protein Motors -- from what we can measure to what we like to know Hongyun Wang Department of Applied Mathematics and Statistics University of.
The Mantle Flow Field beneath Western North America Silver and Holt, Science 295, 1054, 2002 Abigail L. Bull Earthscope Seminar, January 2007.
CHE/ME 109 Heat Transfer in Electronics
Multiple-scale Variability in the Southern California Bight Oceanic Current System Changming Charles Dong Institute of Geophysical and Planetary Physics,
Gravity: Gravity anomalies. Earth gravitational field. Isostasy. Moment density dipole. Practical issues.
Assessment of OIB 2009 Data over Pine Island and Thwaites Glaciers K. Jezek OIB Science Team Meeting.
Introduction to Convection: Flow and Thermal Considerations
Forces Acting on a Control Volume Body forces: Act through the entire body of the control volume: gravity, electric, and magnetic forces. Surface forces:
Chapter 9 Solids and Fluids. Solids Has definite volume Has definite volume Has definite shape Has definite shape Molecules are held in specific locations.
Stress, Strain, and Viscosity San Andreas Fault Palmdale.
Measurement of Kinematics Viscosity Purpose Design of the Experiment Measurement Systems Measurement Procedures Uncertainty Analysis – Density – Viscosity.
WAIS Prediction: Things We Need to Find Out R.B. Alley, S. Anandakrishnan, R.T. Walker, B.R. Parizek, T.K. Dupont, and D.Pollard, Penn State now or in.
Flow and Thermal Considerations
Roland Burgmann and Georg Dresen
Glacier hydrology Ice -directed drainage Isdirigert drenering
Optimization of pocket design for extrusion with minimal defects Kathirgamanathan, P., Neitzert, T.
Astenosphere entrainment at a subduction zone: numerical and laboratory experiments J. Hasenclever*, J. Phipps Morgan †, M. Hort*, L. Rüpke ‡ * Institut.
Conservation of Mass D=Domain of a body of water Water is flowing in and out of D Mass is neither created nor destroyed Flow coming in = Flow going out.
Reynolds Number (Re) Re = R = A/P V = mean velocity  /  =  (which is kinematic viscosity) Re = VR(  /  ), where Driving Forces Resisting Force Re.
FORWARD AND INVERSE MODELLING OF GPS OBSERVATIONS FROM FENNOSCANDIA G.A. Milne 1, J.X. Mitrovica 2, H.-G. Scherneck 3, J.L. Davis 4, J.M. Johansson 3,
Better Physics in Embedded Ice Sheet Models James L Fastook Aitbala Sargent University of Maine We thank the NSF, which has supported the development of.
Sea Ice Deformation Studies and Model Development
Stability and drainage of subglacial water systems Timothy Creyts Univ. California, Berkeley Christian Schoof U. British Columbia.
PTT 204/3 APPLIED FLUID MECHANICS SEM 2 (2012/2013)
A WAIS Analog Found on Mars Polar Cap Weili Wang 1, Jun Li 1 and Jay Zwally 2 1. Raytheon ITSS, NASA/GSFC, Code 971, Greenbelt, MD 20771, USA. 2. Ocean.
Practical Applications Wind Turbine Hydropower Turbine The motion of a fluid is altered so that propulsive forces can be generated on the devices. The.
Elevation Change Anomalies in West Antarctica - New Windows Into Dynamics of Subglacial Water Flow S. Tulaczyk, UCSC L. Gray, CCRS I. Joughin, APL, UW.
Towards repeat-track measurements of elevation change using ICESat/GLAS B. E. Smith Funded by the ICESat science team With thanks to Charlie Bentley, Charlie.
©2010 Elsevier, Inc. 1 Chapter 7 Cuffey & Paterson.
Rheology of the Earth. Schedule Rheology Viscous, elastic & plastic Viscous, elastic & plastic Deformation maps and “Christmas tree’s” for mantle & lithosphere.
Modelling the evolution of the Siple Coast ice streams. Tony Payne 1*, Andreas Vieli 1 and Garry Clarke 2 1 Centre for Polar Observation and Modelling,
Numerical Simulations of Silverpit Crater Collapse: A Comparison of TEKTON and SALES 2 Gareth Collins, Zibi Turtle, and Jay Melosh LPL, Univ. of Arizona.
Warm ocean is eroding WAIS 1 st OctoberWAIS 2004 Slide 1 Andrew Shepherd 1, Duncan Wingham 2, Eric Rignot 3 1 Scott Polar Research Institute 2 University.
Scientific Basis The mission of CReSIS is to develop technologies; conduct field investigations; compile and analyze data to characterize ongoing rapid.
WHOI -- AOMIP 10/20/2009 Formation of the Arctic Upper Halocline in a Coupled Ocean and Sea-ice Model Nguyen, An T., D. Menemenlis, R. Kwok, Jet Propulsion.
Control of Ice Stream Stick-Slip Mechanics by Frictional Healing J. Paul Winberry, Sridhar Anandakrishnan, Chris Marone, Richard Alley, and Don Voigt Penn.
Fluid Flow in Rivers Outline 1.Flow uniformity and steadiness 2.Newtonian fluids 3.Laminar and turbulent flow 4.Mixing-length concept 5.Turbulent boundary.
29 September 2009WAIS/Pack Forest Conference Center Variation in Subglacial Roughness in West Antarctica: How do we interpret causality in the context.
Data source: I. Joughin, JPL G. Catania, H. Conway, C. Raymond and T. Scambos * Earth and Space Sciences, University of Washington, Seattle WA, *
©2010 Elsevier, Inc. 1 Chapter 11 Cuffey & Paterson.
Late breaking news from field studies of the Ross Ice Shelf Douglas R. MacAyeal, Olga Sergienko, Kelly Brunt, Marianne Okal, Jonathan Tom, Ronald Ross,
Modelling Postseismic Deformation: Examples from Manyi, Tibet and L’Aquila, Italy Marcus Bell COMET Student Meeting 2010 Supervisors: B. Parsons and P.
Validation of physics-based ground motion earthquake simulations using a velocity model improved by tomographic inversion results 1 Ricardo Taborda, 1.
An example of vertical profiles of temperature, salinity and density.
Better Physics in Embedded Models: Iceberg arcing and Lake-surface profiles Aitbala Sargent, James L Fastook, Ted Scambos. University of Maine We thank.
Sediments, Water, and Inland Ice Flow: A Geologic Control on Ice Stream Tributaries? Leo E. Peters Sridhar Anandakrishnan, Richard B. Alley, J. Paul Winberry,
Canada Centre for Remote Sensing Earth Sciences Sector Influence of ice dynamics on firn layer stratigraphy Laurence Gray (1), Ed King, (2), Howard Conway.
Estimating surface elevation changes on WAIS from GLAS altimetry Ben Smith U of W 9/30/04.
Abj 4.2.2: Pressure, Pressure Force, and Fluid Motion Without Flow [Q2 and Q3] Area as A Vector Component of Area Vector – Projected Area Net Area.
Louisiana Tech University Ruston, LA Boundary Layer Theory Steven A. Jones BIEN 501 Friday, April
Derivative-based uncertainty quantification in climate modeling P. Heimbach 1, D. Goldberg 2, C. Hill 1, C. Jackson 3, N. Petra 3, S. Price 4, G. Stadler.
Geopotential and isobaric surfaces
A Generalized Ekman Model for Frontal Regions Meghan F. Cronin William S. Kessler NOAA Pacific Marine Environmental Laboratory Cronin, M.F. and W.S. Kessler.
MTH- 486: Fluid Mechanics Instructor: Dr. Fahad Munir Abbasi Assistant Professor Department of Mathematics Comsats Institute of Information Technology.
1D Hydraulic Modeling w/ LiDAR Data Noah J. Finnegan 1 1 UC Santa Cruz, Earth & Planetary Sciences.
Fracture Toughness of Metallic Glasses: A Ductile-to-Brittle Transition? Eran Bouchbinder Weizmann Institute of Science Work with Chris H. Rycroft University.
Towards the utilization of GHRSST data for improving estimates of the global ocean circulation Dimitris Menemenlis 1, Hong Zhang 1, Gael Forget 2, Patrick.
Overview of processes Module 8.
Asthenosphere flow and mantle lithosphere instabilities below continental rifts and rifted margins Jolante van Wijk (University of Houston) Jeroen van.
Presentation transcript:

Basal Shear Stress of the Ross Ice Streams from Control Method Inversions Ian Joughin Jet Propulsion Lab, California Institute of Technology Slawek Tulaczyk University of California, Santa Cruz Douglas R. MacAyeal Dept. of Geophysical Sciences, University of Chicago

Mercer Whillans Kamb Bindschadler MacAyeal A B C D E

Ice Stream Motion Over a Till Bed Ice ~1000 m Till ~6 m Depth Velocity Depth Velocity Viscous Deforming Bed ( Alley,Blankenship et al ) Weak Plastic Bed ( Kamb,Tulaczyk,Engelhardt et al )  A weak bed implies inability to support high driving stress

Ice Stream Equations Viscous Plastic  Control-method techniques can be used to invert equations for basal shear stress (MacAyeal, 1992).

Similar solutions for both plastic and viscous models (force balance). Inversions are robust with respect to errors in velocity and bed topography. Inversions are sensitive to surface elevation noise Inversion Result Forward Model Noise Inversion Procedure Inversion Simulations

Bed Elevation - BEDMAP Data Sets Surface Elevation – RAMP/SOAR B – Temperature Model

Ice Streams A&B

Ice Stream C

Ice Streams D&E

Weak Margins ?

Summary  Fairly uniform weak (few kPa) bed beneath ice streams (E has significant sticky spots).  Tributaries a mixture of strong and weak bedded regions.  Some ambiguity in basal shear stress because flow law not well constrained.  Neither model nor data appear to support weak margins.