GLOBAL TOPOGRAPHY CONTINENTAL & OCEANIC LITHOSPHERE CONTINENTAL & OCEANIC LITHOSPHERE Age Topography mid ocean ridge mantle Heat Flow tectothermal age of plate (ta) MOR t mantle flow mantle heat loss (q ) thermal Thermal boundary layer of mantle convection t Ts Ts To t=0+ time t=0 z _ z To Region of T gradient is a Thermal Boundary Layer tectothermal age of plate (ta) MOR c m t mantle flow mantle heat loss (q ) thermal Thermal boundary layer of mantle convection t mechanical m : Layer of long term strength (cold=hi viscosity) chemical/mechanical m : Dehydrated Layer (dry=hi viscsoity) Continent Oceanic Thermal Lithosphere defines convection pattern - it is the cold, overturning boundary layer. Oceanic Chemical Lithosphere subducts - overturning portions of the Earth see a constant temperature boundary condition. Continental Chemical Lithosphere does not participate in convective mantle overturn (inherently buoyant). Provides a more complex thermal coupling condition for covecting mantle below. Cooper et al. 2004 convecting mantle cold hot failed region extension upper crust lower crust cratonic root bulk mantle failed region compression local geotherm warm mantle viscosity = 10 21 Pa s “subducting” lithosphere viscosity = 10 25 Pa s Cooper et al. 2004 Chemical/Mechanical Lithosphere Dynamic Mantle Sub-Layer Thermal Lithosphere t c 0 surface heat flow Upper Crust Lower Crust Depth (km) 50 mantle heat flow 100 150 200 Chemical Lithosphere Average Thermal Lithosphere 250 300 0 200 400 600 800 1000 1200 1400 Temperature (Celsius) c t Thermal/Chemical BL Thickness Ratio 700 4 600 3.5 500 3 Radiogenically Depleted Root 400 2.5 Radiogenically Enriched Root 2 300 200 1.5 100 1 40 60 80 100 120 140 160 180 200 Chemical Boundary Layer Thickness (km) Temperature Drop Across Sub-Layer (C) 4.5 QuickTime™ and a decompressor are needed to see this picture. Chem Therm 65 60 55 50 Latitude Yuan & Romanowicz 2010 45 40 35 Thermal/Chemical Ratio Preserving Destroying The&Structure of Cratonic Lithosphere 4 3 2 50 100 150 200 Chemical Lithosphere (km) CRATON INSTABILITY STABILITY Preserving & Destroying Cratonic Lithosphere UNDERSTAND STABILITY TO UNDERSTAND INSTABILITY MODELING CRATON STABILITY chemically real light material - crust (has own rheology) mantle cold hot failed regions chemically light material - root (own rheology) cold viscosity 10 26 Pa s 21 hot viscosity 10 Pa s base of thermal lithosphere continental lithosphere is cool & more viscous than bulk mantle MODELING CRATON STABILITY Send Continent into Model Subduction Zone See What it Takes to Save Root & Keep Crust Stable 300+ Simulations Later … MODELING CRATON STABILITY - BUOYANCY Buoyancy Does Not Lead To Stability (even w/ temperature dependent viscosity) 7 Myr 29 Myr MODELING CRATON STABILITY - VISCOSITY Root 1000X Viscosity of Mantle at = Temp Viscosity Does Not Lead To Stability 50 Myr 100 Myr Viscosity+ Critical Thickness Can Lead To Stability MODELING CRATON STABILITY - VISCOSITY Normalized Root Extent Extreme De-Hydration 1.0 Root/Mantle Viscosity Ratio = 1000 0.8 0.6 50 Myr 100 Myr 150 Myr 0.4 0.2 120 140 160 180 200 250 Root Thickness (km) Lower Ratio (>100) Can Not Prevent Viscous Root Deformation MODELING CRATON STABILITY - VISCOSITY Root 1000X Viscosity of Mantle at = Temp Viscosity Does Not Lead To Stability 50 Myr 100 Myr Viscosity+High Craton Yield Stress Can Lead To Stability MODELING CRATON STABILITY - YIELD STRESS Normalized Root Extent 1.0 Root & Crust; 50myr Root & Crust; 100myr Root Only; 50Myr Root Only; 100Myr 0.8 0.6 0.4 0.2 0.1 1.0 0.15 0.2 0.25 0.3 0.35 1.5 2.0 2.5 3.0 3.5 Continent/Mantle Yield Ratio 0.4 4.0 Craton Does Not Fail Under Stress Due to High Yield Strength Buffer Cratons from High Stress and They Will Not Yield Auto makers consider it impractical to make drivers heads stronger so ……... MODELING CRATON STABILITY - MOBILE BELTS Mobile Belts Can Provide Craton Stability (act as crumple zones to buffer stress) 50 Myr 100 Myr REGENERATING MOBILE BELTS (Crumple Zones) if subduction starts offshore, forms island arc, then migrates on shore - craton will be buffered if subduction starts at time B - craton will be stressed crumple zone model mobile belt (deep green) yield stress relative to craton (pale green) yield = 0.5 craton craton no crumple zone yield ratio = 0.5 yield ratio = 1.0 INSTABILITY Dry Viscosity/Thickness Rehydrate/Thin from Below High Yield Stress Rehydrate Mobile Belt Stress Buffers Lack of Buffer Precambrian Palaeozoic barren Silurian diamond kimberlite volcanism kimberlite Mesozoic Basin development/volcanism Cenozoic Volcanism and extension Archean crust (3800 Ma) Loss of > 120 km of Archaean lithosphere, Sino-Korean craton S-K C Asthenosphere (1300 C) Asthenosphere (1300 C) Asthenosphere (1300 C) Asthenosphere (1300 C) crust removed cratonic root cratonic root Low Angle Subduction Would Allow For Rehydration Weakening S-K C Why Geologically Recent Instability ? Weakening Elements in Place in Past INSTABILITY Increasing Mantle Stress Horizontal Surface Velocity Failure Zone Subducting Slab Track Temperature, Strain Rate, and Stress Profiles To Get Average Lithospheric Stress Gives a Measure of Convective Mantle Stress Vary Internal Heating To See How Mantle Stress Varies With Convective Vigor INCREASE INTERNAL HEATING DECREASE MANTLE VISCOSITY 375 4 Lithospheric Stress (Mpa) 1.5 10 Lower Viscosity Dominates Stress Scaling 4 1 10 250 5000 125 00 0 5 6 5x10 10 7 1x10 15 20 7 2x10 Internal Heating Rayleigh Number MODELING CRATON STABILITY O’Neill et al., Lithos (2010) Vary Cratonic Properties: Viscosity, Yield Stress, Buoyancy Vary Mantle Properties: Clayperon Slope, Upper/Lower Mantle Viscosity, Convective Vigor (increases in past) Dehydrated Craton Stress (Mpa) Mantle Heat Production Weakened (Hydrated) Craton Large Disruption, Recycling Weakened (Hydrated) Craton Small Disruption, No Recycling 4 4 1 10 5000 Craton Yield Stress (Mpa) Mantle Stress (Mpa) 1.5 10 Reference (dry) Weakened (rehydrated) 0 0 Past 5 10 15 Present Geologic Time 20 Future High Craton Viscosity Leads to Stability in Thick Root Limit. INSTABILITY: Rehydrate to Lower Viscosity High Yield Stress Relative to Ocean & Peripheral Continental Lithosphere Leads to Stability INSTABILITY: Lower Yield Stress (water) or No Peripheral Buffer Mantle Stress Can Increase Over Time Due To Increasing Mantle Viscosity Greater Potential for INSTABILITY in Geologic Present Vs. Ancient Past