Evolution of Wedge Width Dampens the Response of Rock Uplift Rate to a Change In Fa (from linear to ~1/2 power) A Step-function change in U Is nearly impossible.

Slides:



Advertisements
Similar presentations
1 Wake Fields and Beam Dynamics Kai Meng Hock. 2 Overview Research Interests –Wake fields Electromagnetic fields are induced by charged particles interacting.
Advertisements

Application of the fission track method in Geology Part - II.
GE177b- Objectives Introduce a variety of techniques to describe ‘quantitatively’ deformation of the lithosphere and fault slip history. Introduce.
1 Characterizing the Impact of Horizontal Heat Transfer on the Linear Relation of Heat Flow and Heat Production Ronald G. Resmini Department of Geography.
Objectives Describe the elevation distribution of Earth’s surface.
EROS (Crave & Davy, 2001) “Stochastic model of erosion– sedimentation processes, based on cellular automata, which mimics the natural variability of climatic.
LOCALIZATION OF SEDIMENTARY ROCKS DURING DUCTILE FOLDING PROCESSES Pablo F. Sanz and Ronaldo I. Borja Department of Civil and Environmental Engineering.
Semi-alluvial channels GBR 7, Tadoussac 2010 Semi-alluvial channels and sediment-flux-driven bedrock erosion Jens M. Turowski With thanks to: D. Lague,
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.
Design Optimization of Longwall Chain Pillars
Leech Heart Half- Center Oscillator: Control of Burst Duration by Low- Voltage Activated Calcium Current Math 723: Mathematical Neuroscience Khaldoun Hamade.
Critical Wedge Taper: Kinematic Response to Surface Processes and Relation to Sevier Orogeny Tarka Wilcox Image: Google Earth, Taiwan.
Weismann (1992) Weisman, M. L., 1992: The role of convectively generated rear- inflow jets in the evolution of long-lived mesoconvective systems. J. Atmos.
ROLE OF HEADLANDS IN LARVAL DISPERSAL Tim Chaffey, Satoshi Mitarai Preliminary results and research plan.
Ge/Ay133 How do small dust grains grow in protoplanetary disks?
Collisional ionization in the beam body  Just behind the front, by continuity  →0 and the three body recombination  (T e,E) is negligible.
Announcements Field trip this Saturday to Collosal Cave area 7:30 AM at loading dock. We will map some really cool stuff! Please review map symbols and.
(Chapter 10 in D & R) Geometry and Kinematics: Plates.
Himalayan foreland Foreland basins
Alessandro Cappelletti for CTF3 collaboration 5 th May 2010 RESULTS OF BEAM BASED RF POWER PRODUCTION IN CTF3.
Earthquake nucleation How do they begin? Are large and small ones begin similarly? Are the initial phases geodetically or seismically detectable? Related.
Atmospheric Force Balances
8.8 Energy Transfer within the Climate System. Air and Ocean Circulation  Sun hits earth at different intensities and latitudes  Water and land absorb.
mountains, mountain building, & growth of continents
Simulation Output Analysis
Analyzing the systemic function of genes and proteins Rui Alves.
Feedbacks between mountain building, erosion and climate
Timothy Reeves: Presenter Marisa Orr, Sherrill Biggers Evaluation of the Holistic Method to Size a 3-D Wheel/Soil Model.
Influence of Magma on Rift Evolution: A Modeler’s Perspective Mark D. Behn Department of Geology & Geophysics, Woods Hole Oceanographic Institution Roger.
Nicole Gasparini Arizona State University Landscape Modeling.
Structure of a Continent Figure How are continental plates formed? Figure 13-4.
Geomorphology GLG362/598 Instructor: Kelin X. Whipple, ISTB4-777 TA: Andrew Darling, ISTB4-
The Impact of Orographic Precipitation on the Form of Mountain Ranges Alison Anders Earth and Space Sciences Dale Durran Atmospheric Sciences Gerard Roe.
Numerical models of landscape evolution Mikaël ATTAL Marsyandi valley, Himalayas, Nepal Acknowledgements: Jérôme Lavé, Peter van der Beek and other scientists.
Numerical simulations of thermal counterflow in the presence of solid boundaries Andrew Baggaley Jason Laurie Weizmann Institute Sylvain Laizet Imperial.
GEO-4840 TECTONICS-S05 PART 1: LECTURES [ Wed (16) ] 19/1 - 09/3 PART 2: STUDENT PROJECTS [ Presentations ] 13/4 PART 3: FIELD TEACHING [ Corsica.
Laurent G. J. Montési Maria T. Zuber ASME, 1999 The importance of localization for the development of large-scale structures in the Earth’s crust.
Simulating Glacial Erosion Using Landscape Evolution Code Chelsea Willett EPS 109 – Fall 2014.
External Modulator. When data rates were in the low gigabit range and transmission distances were less than 100 km or so, most fiber optic transmitters.
Aim: How are landscapes defined? Do Now: Try to define the following vocabulary terms in your own words or try to give descriptions of what these landscapes.
Modelling of the motion of phase interfaces; coupling of thermodynamics and kinetics John Ågren Dept of Materials Science and Engineering Royal Institute.
How’s it going to end? Climate evolution on Mars and Venus and its bearing on the very long term fate of the Earth’s climate system.
Arcs and global biogeochemical cycles Louis Derry Cornell University How does weathering, erosion and geothermal activity in arc terranes impact global.
© The McGraw-Hill Companies, 2005 EDUCATION AND GROWTH: THE SOLOW MODEL WITH HUMAN CAPITAL Chapter 6 – second lecture Introducing Advanced Macroeconomics:
Erosional Features (Typical of Active Margins)
Denali By Gary Cutler. How it was formed and where it is Denali was formed by erosion and frequent earthquakes, also the mountains were formed by the.
Tune: Decay at Injection and Snapback Michaela Schaumann In cooperation with: Mariusz Juchno, Matteo Solfaroli Camillocci, Jorg Wennigner.
Presented by: Khiem Phan. OUTLINE I. Introduction II. Materials and Methods III. Results IV. Conclusions
U NIVERSITY OF S CIENCE AND T ECHNOLOGY OF C HINA Influence of ion orbit width on threshold of neoclassical tearing modes Huishan Cai 1, Ding Li 2, Jintao.
Aim: How are landscapes defined? Do Now: Try to define the following landscapes in by giving descriptions and facts that characterize each landscape. 1)
River Incision into Bedrock Interaction of a suite of processes Plucking, Abrasion (bedload & suspended load), Cavitation (?), Weathering Vortices shed.
Lecture Outlines Physical Geology, 14/e
Lecture Outlines Physical Geology, 10/e
But, classic Plate Tectonics do not explain everything…
LANDSCAPE DEVELOPMENT
Mountain Building “Tectonic Forces at Work”
Multiscale aspects of cloud-resolving simulations over complex terrain
Morphodynamic and Sediment Tracers in One-Dimension
Are these interesting questions?
DETRITAL ZIRCON RECORD
The Interannual variability of the Arctic energy budget
Aim: How are landscapes defined?
Advanced Macroeconomics:
Chapter 22.
Coronal Loop Oscillations observed by TRACE
Geomorphology GLG362/598 Instructor: Kelin X. Whipple, ISTB4-777 (5-9508) TA: Emily Zawacki, ISTB4-603 Office Hours – just.
Ahmed Ibrahim Kazunari Shibata Kwasan Observatory, Kyoto University
Harry Williams, Geomorphology
Role of subducted sediments in plate
Presentation transcript:

Evolution of Wedge Width Dampens the Response of Rock Uplift Rate to a Change In Fa (from linear to ~1/2 power) A Step-function change in U Is nearly impossible Total Erosional Efflux can only change during Transients; Only Climate can Drive a Spike A Change in Erosional Efficiency Changes both Relief AND the Steady- State Rock Uplift Rate: Coupling Between Erosion and Tectonics Response Time Set by Final Erosional Efficiency (~only) Persistent  U

Taiwan Central Range GTOPO30 DEM Time Since Collision Increases at ~1Ma/60 km from south

Taiwan Central Range 20 km Averaging Time Since Collision Increases at ~1Ma/60 km from south Notable Departure from Steady Self-Similar Growth

Taiwan Topography – Approach to Steady State (Willett et al) Distance = Time (Oblique convergence) 130km = Ma

Taiwan Central Range not Consistent with Self-Similar Growth But predicted time to steady state approximately corroborated

Taiwan Central Range Parameters Time to 90% Steady- State Values much shorter for Rock Uplift and Erosion Rate T 1/e ~ 1.2 Ma 90% Steady-State Wedge Size, Erosional Flux ~3Ma During Early stages of growth, Rock Uplift and Erosion follow very distinct paths x longer if dry, harder rock

Conclusions: Frictional Orogenic Wedges Response Time Set by Erosional Efficiency T 1/e ~ order 1Ma typical for wet climate, moderate rock strength (Taiwan example) Fast response to increase K*, Moderate response to change F A, Slow response to decrease K* Implusive (nearly 1:1) transient response of rock uplift to increase K* : isostatic For growing wedge, rock uplift and erosion rate approach near steady values long before wedge attains flux steady-state

The Erosion and Rock Uplift Paradox In an isostatically compensated orogen, most (~5/6 total) rock uplift can be said to be a response to erosion At steady state, rock uplift equals erosion – the two are interchangeable Thus it makes no sense to discuss how erosion influences rock uplift – rock uplift is erosion, more or less If erosion is not driven by rock uplift, but vice versa, what does drive erosion? And how is relief generated? Did Someone Say Something about a Paradox?

Suggested Language Erosion  Tectonics Erosion  Rock Uplift Erosional Efficiency  Rock Uplift Erosion  Rock Deformation

But What Do We Really Know? Wedge Theory, Coupled Numerical Simulations, and Analog Models Suggest a Strong, Inescapable Coupling between Erosional Efficiency and Tectonics (rock deformation rates, patterns, PTt histories of exposed rocks) But: Quantitative link between Climate Parameters and “Erosional Efficiency” remains Elusive There is yet no Field Data that Convincingly Demonstrates a Strong Coupling, with Feedback, between Climate and Tectonics Many are Pursuing this Goal; much existing data is tantalizing/ suggestive. Willett: Alps Messinian Crisis?