5868 Dan Tatham

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Microstructure evolution Microstructure evolution during creep and during creep and annealing of minerals annealing of minerals and rocks and rocks Microstructure evolution Microstructure evolution during creep and during creep and annealing of minerals annealing of minerals and rocks and rocks 1 D. Tatham, D.J. Prior, E. Mariani, S.J. Covey- Crump, J. Mecklenburgh, J. Wheeler

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Microstructure evolutionMicrostructure evolution

during creep andduring creep andannealing of mineralsannealing of mineralsand rocksand rocks

Microstructure evolutionMicrostructure evolution

during creep andduring creep andannealing of mineralsannealing of mineralsand rocksand rocks

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D. Tatham,D.J. Prior, E. Mariani, S.J. Covey-Crump, J. Mecklenburgh, J. Wheeler

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High temperature deformation in the EarthHigh temperature deformation in the EarthHigh temperature deformation in the EarthHigh temperature deformation in the Earth

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Ed Garnero 

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How do we gain insight into mechanisms of

deformation in the Earth’s crust and their implications?

SE NWTorre Saliere

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Fold structure in theFold structure in the MorcleMorcle NappeNappe,, SalanfeSalanfe, Swiss, SwissAlpsAlpsFold structure in theFold structure in the MorcleMorcle NappeNappe,, SalanfeSalanfe, Swiss, SwissAlpsAlps

1 Km

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Naturally deformed systems

 

Electronbackscatter

diffraction(EBSD)

Tools for understanding high temperatureTools for understanding high temperaturedeformation of rocksdeformation of rocks

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“Final microstrucutres ”

Experimental

rockdeformation

“Post mortem 

analysis ”

Modelling

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These may tell us about:

•  

We track microstructural evolutionthrough in-situ heating and deformationexperiments in the SEM with

simultaneous EBSD

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• the behaviour of special (twin, CSL) boundaries

• the control of orientation/chemistry on boundary migration

• what mechanisms control static and dynamic recrystallization

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The SEM in LiverpoolThe SEM in LiverpoolThe SEM in LiverpoolThe SEM in Liverpool

• The CamScan X500CrystalProbe is specificallydesigned for high-temperature in situ experiments.

• Tilted column permitsexperimentation on horizontal

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• Sample assembly anddetectors separated bywater-cooled heat shield,reducing contamination ofsignal at high experimentaltemperatures.

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Static Heating StageStatic Heating StageStatic Heating StageStatic Heating Stage

• Coiled Ta wire resistanceheater.

• Capable of furnace

temperatures in excess of1200oC.

• Equates to sample surfacetemperatures in excess of

o

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• Samples up to 9x9x3mm sit ina cavity in graphite furnacecore.

• Furnace heating path controlled

by a Oxford InstrumentsIntelligent TemperatureController.

Seward et al., 2000 Scanning , 24, 232-240.

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Annealing of deformed NaClAnnealing of deformed NaClAnnealing of deformed NaClAnnealing of deformed NaCl

8Bestmann et al., 2005. J. Struct. Geol. 47, 447-457 Piazolo et al. 2006, Tectonophysics 427, 55-71

Slide8.avi 

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Before heating

Annealing of deformed NaClAnnealing of deformed NaCl

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500 µµµµmBestmann et al., 2005. J. Struct. Geol. 47, 447-457 

Piazolo et al. 2006, Tectonophysics 427, 55-71

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after 4.5h heating at 350-410°°°°C

Annealing of deformed NaClAnnealing of deformed NaCl

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500 µµµµm

Bestmann et al., 2005. J. Struct. Geol. 47, 447-457 

Piazolo et al. 2006, Tectonophysics 427, 55-71

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GBM at low T GBM at high T

12 Piazolo et al., 2006, Tectonophysics 427, 55-71

Increasing length of straight segment movement

Increasing face control

Decreasing influence of pre-existing substructure

Decreasing tendency to create ‘poikiloblasts’

Increasing continuity (time and space) of movement

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Grain growth in annealed copper at 850Grain growth in annealed copper at 850ooCCGrain growth in annealed copper at 850Grain growth in annealed copper at 850ooCC

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Video is 30x real-time

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Grain growth in annealed copper at 850Grain growth in annealed copper at 850ooCCGrain growth in annealed copper at 850Grain growth in annealed copper at 850ooCC

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In In- -situ situ deformation & heating stagedeformation & heating stageIn In- -situ situ deformation & heating stagedeformation & heating stage

• Stepper motor-driven tensileheating/deformation rig in-situ in SEM.

• Opposing lead screws allowtensile load & strain whilekeeping the area of investigationunder the electron beam.

 

LVDTs

Load

cell

Steppermotor

Sample

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capable of furnacetemperatures in excess of1400oC & sample surfacetemperatures well in excess of1000oC.

• Samples thermally isolated fromdeformation assembly byceramic jig.

• Controlled via LabVIEW.

Water-cooled plate

HeatersCeramic sample jig

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Deformation in copper at ~700Deformation in copper at ~700ooCCDeformation in copper at ~700Deformation in copper at ~700ooCC

16Video is 300x real-time, 0.8mm total extension

Slide16.avi 

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P,T

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Pressure

• inhibits brittle failure

• promotes GBM

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In the SEM we need higher temperature but...

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Practicalities of working on geologically important materialsPracticalities of working on geologically important materials

20Mariani and Tatham, unpublished experiments; Bestmann. unpublished experiments 

Slide20.avi 

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LVDT

fixed piston

displacement rods

Tracking microstructure evolutionTracking microstructure evolution

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High T creep rig 

(to Mariani, July 09) 

New SEM stage 

(to Prior, January 09) passive load

moving piston

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microstructural evolution

Tracking microstructure evolutionTracking microstructure evolution

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shear strain      s       t      r      e

      s      s

rheology 

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U n d e f o r m e d

Tracking microstructure evolutionTracking microstructure evolution

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5 0 0 1 0 0 0

s c a l e / m s c a l e / m

00 5 0 0 1 0 0 0

shear strain = 0.5

 T=973K 

P = 3 0 0 M P a

With Julian Mecklenburgh,

Manchester 

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Higher ResolutionHigher ResolutionHigher ResolutionHigher Resolution

Carrara marble

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Solenhofen limestone

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Thank you

 

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pcwww.liverpool.ac.uk/~tatham/mtmovies.zip