Investigation of the texture and microstructure evolution around a nanoindent close to an individual grain boundary. David Mercier1 (d.mercier@mpie.de),

Slides:



Advertisements
Similar presentations
Department of Microstructure Physics and Metal Forming Düsseldorf, Germany Piling-up behavior during axisymmetric indentation and its.
Advertisements

Crack Nucleation and Propagation
Presented by: Nassia Tzelepi Progress on the Graphite Crystal Plasticity Finite Element Model (CPFEM) J F B Payne L Delannay, P Yan (University of Louvaine)
Incubation & Nucleation Validation Study SIPS TIM, October 22 nd 2007 Cornell and RPI.
Chapter 6 Geometry of Deformation and Work-Hardening.
Deformation and Recrystallization of Mg Alloy AZ31 M.A.Sc: Shenglong Liang Supervisor: Hatem S. Zurob.
The effect of crystal orientation on the indentation response of commercially pure titanium: experiments and simulations by T. B. Britton, H. Liang, F.
ASE324: Aerospace Materials Laboratory Instructor: Rui Huang Dept of Aerospace Engineering and Engineering Mechanics The University of Texas at Austin.
Fatigue Initiation Makes up some 90% of the total fatigue life Little has been understood about it Experimental fatigue testing of components is very costly.
MCP 1 L. Zhang and M. T. Lusk Colorado School of Mines T.J. Bartel and E.A. Holm Sandia National Laboratories March 18, 2008 Anisotropic EBSD Nickel data.
HIGH-STRAIN-RATE BEHAVIOR OF POLYCRYSTALLINE  -IRON D. Rittel, M. Vural, M. Tao, S. Mizrach, A. Bhattacharyya, G. Ravichandran SPECIMEN GEOMETRY and MATERIAL.
Role of Deformation Twinning in Strain Hardening and Texture Evolution: Experiment and Numerical Simulation S. R. Kalidindi & R. D. Doherty, Drexel University,
Dislocations and Strengthening
Princeton University Department of Mechanical and Aerospace Engineering The Effect of Inclination on Grain Boundary Mobility Hao Zhang; Mikhail I. Mendelev;
Graduate Seminar I Compositionally Graded High Manganese Steels by Morteza Ghasri Supervisor: Prof. McDermid Nov. 18, 2011.
Crystallographic Aspects of Dislocations
Minimum Grain Size in Nanostructured Materials Produced by Cryomilling NSF Grant MET DMR Farghalli A. Mohamed and Yuwei Xun University of California,
1 /52 The Hall-Petch Relationship in cast Mg and Mg-Zn Solid Solutions C.H. Cáceres, Gemma E. Mann, J.R. Griffiths a Co-operative Research Centre CAST.
Anisotropy of Commercially Pure Titanium (CP-Ti) Experimental Setup and Procedures Experimental Results Results and Conclusions Project Objective: To assess.
Irradiation study of Ti-6Al-4V and Ti-6Al-4V-1B for FRIB beam dump:
DISLOCATION MOVEMENT.
C. Keller, L. Duchêne, M. Afteni, E. Hug, A-M Habraken 2-4 June 2010 ICACM Paris France.
COMING FROM? IMDEA Materials Institute (GETAFE) Polytechnic University of Madrid Vicente Herrera Solaz 1 Javier Segurado 1,2 Javier Llorca 1,2 1 Politechnic.
Deformation Twinning in Crystal Plasticity Models
Nicholas Zabaras (PI), Swagato Acharjee, Veera Sundararaghavan NSF Grant Number: DMI Development of a robust computational design simulator for.
Byeong-Joo Lee Byeong-Joo Lee Micro Monte Carlo Simulation - Literature (from N.M. Hwang) 1. “Texture.
A Multi-Scale Mechanics Method for Analysis of Random Concrete Microstructure David Corr Nathan Tregger Lori Graham-Brady Surendra Shah Collaborative Research:
The Structures of Metals
Department of Tool and Materials Engineering Investigation of hot deformation characteristics of AISI 4340 steel using processing map.
Max-Planck-Institut für Eisenforschung, GmbH Highly localized slip traces observed near grain boundaries on slip systems with lower (global) Schmid factors.
J. L. Bassani and V. Racherla Mechanical Engineering and Applied Mechanics V. Vitek and R. Groger Materials Science and Engineering University of Pennsylvania.
2D Crystal Plasticity.
A probabilistic twin nucleation model for HCP polycrystalline metals
Bin Wen and Nicholas Zabaras
Equal Channel Angular Pressing of High Purity Aluminum Julio A. Nunez Chris Hovanec Dr. Surya R. Kalidindi Dr. Roger D. Doherty Mechanics of Microstructures.
FAMU-FSU College of Engineering Department of Mechanical Engineering 1 ORIENTATION IMAGING MICROSCOPY (OIM) - SOME CASE STUDIES EML 5930 (27-750) Advanced.
Crystal Plasticity Class One.
Materials Process Design and Control Laboratory Finite Element Modeling of the Deformation of 3D Polycrystals Including the Effect of Grain Size Wei Li.
Uncertainty quantification in multiscale deformation processes Babak Kouchmeshky Nicholas Zabaras Materials Process Design and Control Laboratory Sibley.
Meso-Scale Simulation and Measurement of Dislocation/Grain Boundary Interactions AFOSR Grant Number: FA , 0088 Robert H. Wagoner, PI, Myoung-Gyu.
Multi-scale Modeling of Nanocrystalline Materials
1. Introduction Assoc.Prof.Dr. Ahmet Zafer Şenalp Mechanical Engineering Department Gebze Technical.
Single-Crystal Elastic Constants of High-Manganese TWIP Steel Determined by a New Method Utilizing Nanoindentation James E. Wittig, Vanderbilt University,
Twinning Studies via Experiments and Theory Huseyin Sehitoglu, University of Illinois, DMR The intellectual focus in this work is threefold. The.
Lecture 22: The mechanism of plastic deformation, part 2
Ductile Regime Machining of SiC J. Patten (PI), Western Michigan University, DMR We have previously demonstrated ductile regime machining of SiC.
Deformation and Strengthening Mechanisms of Materials
PLASTIC DEFORMATION Dislocations and their role in plastic deformation.
© 2011 Cengage Learning Engineering. All Rights Reserved Chapter 8: Strain Hardening and Annealing Chapter 8: Strain Hardening and Annealing.
Polycrystal theory and simulation Small scale crystal plasticity
EBSD analysis of dislocations on DC-Spark sample after heat treatment (1.040 C in H 2, 2h) Anité Pérez Fontenla
NUMISHEET2005 —Detroit, MI August 15-19, Cyclic and Monotonic Plasticity of Mg Sheet R. H. Wagoner, X. Lou, M. Li, S. R. Agnew*, Dept. Materials.
25-26 January Bochum, Germany Luc Hantcherli - Philip Eisenlohr - Franz Roters – Dierk Raabe and Collaboration between: Mechanical twinning in crystal.
Tensile Tests on Single Crystal Specimens with Different Orientations D. Kang 1, D. Baars 1, T. Bieler 1, C. Compton 2 1 Michigan State University, East.
Micro-scale single crystal Bauschinger effect and reversible plasticity in copper during bending MRS Fall Conference 1. Dec Boston, USA Düsseldorf,
Monday, February 15, :00p.m. Jacobs Hall Room 298 “A general and predictive model of anisotropic grain boundary energy and morphology for polycrystal-level.
Haidong Liu Mentor: Dr. Peter C Collins, Matt Kenney
Methods (3D EBSD, CP-FEM) Characterization
Grain Boundary Engineering ( Basic Knowledge : Part 2 )
Finite Element Modeling of Nacre
Kristián Máthis1, G. Csiszár2, J. Čapek1, J. Gubicza2, B. Clausen3, P
Piling-up behavior during axisymmetric indentation and its relation to the activated deformation mechanisms in -TiAl C. Zambaldi, S. Zaefferer, F. Roters,
Date of download: 10/25/2017 Copyright © ASME. All rights reserved.
Indira Gandhi Centre for Atomic Research, India
Dislocations and Strengthening
Origin of dramatic oxygen solute strengthening effect in titanium
Visco-plastic self-consistent modeling of high strain rate and
Instructor: Yuntian Zhu
ORIENTATION IMAGING MICROSCOPY (OIM) - SOME CASE STUDIES
Rodrigues–Frank (RF) space or Rodrigues space
Presentation transcript:

Investigation of the texture and microstructure evolution around a nanoindent close to an individual grain boundary. David Mercier1 (d.mercier@mpie.de), C. Zambaldi1, P. Eisenlohr2 M. A. Crimp2, T. R. Bieler2 1Max-Planck-Institut für Eisenforschung, 40237 Düsseldorf, Germany 2Michigan State University, East Lansing, MI 48824, USA 17th International Conference on Textures of Materials August 24-29, 2014 | Dresden, Germany Gr. A Gr. B

Plasticity of Single Crystal is well understood. Motivation of this work Plasticity of Single Crystal is well understood. Indentation experiments are often used to characterize plasticity of single crystal… More complex, but faster, and possible to probe rapidly a lot of GBs, lot of data in a afternoon… Inverse pole figure of pile-up topographies of cp-Ti1 Misorientation maps underneath the indentation at different cross sections, comparison between experimental and simulation results2 Zambaldi C. “Orientation informed nanoindentation of a-titanium: Indentation pileup in hexagonal metals deforming by prismatic slip.”, J. Mater. Res., 2012, 27(1), pp. 356-367. Zaafarani N. “On the origin of deformation-induced rotation patterns below nanoindents.”, Acta Mater., 2008, 56, pp. 31-42. But, missing element to predict polycrystal mechanics… 2014-08-25 MERCIER David

Micromechanical behavior of grain boundaries. Motivation of this work (2/2) Micromechanical behavior of grain boundaries. EBSD and indentations close to grain boundaries are performed in alpha-Ti  quasi bi-crystal deformation. AFM topography of residual indent in Ti-5Al-2.5Sn, close to a grain boundary. Gr. A Gr. B Comparison of experimental results (residual topography, texture around indent…) to simulated indentations as predicted by 3D CPFE modeling. More complex, but faster, and possible to probe rapidly a lot of GBs, lot of data in a afternoon… Start to model the slip transmission and GB mechanic… 2014-08-25 MERCIER David

MATLAB Toolbox and Graphical User Interfaces (GUIs) Strategy  Creation of a toolbox MATLAB Toolbox and Graphical User Interfaces (GUIs) Slip transmission model GB and Bicrystal definition Crystal Plasticity 2014-08-25 MERCIER David

a b nGB Bicrystal definition  5 DOF Geometrical description1,2 Trace of the grain boundary (GB) Geometrical description1,2 GB inclination (b) (by serial polishing or by FIB) and GB trace (a) (by EBSD ) Or GB normal (nGB) Step between grains after polishing / Rougness (by AFM) a b nGB Crystal 1 GB 𝛗 𝟏 𝛟 𝛗 𝟐 𝟏 Crystal 2 𝛗 𝟏 𝛟 𝛗 𝟐 𝟐 𝒖𝒗𝒘 𝝎 Crystallographic description3 Euler angles of grains (12 3) (by EBSD) Or Misorientation axis / angle [uvw] / w (by EBSD or TEM) Randle V. “Five-parameter’ analysis of grain boundary networks by electron backscatter diffraction.”, J. Microscopy, 2005, 222, pp. 69-75. Randle V. “A methodology for grain boundary plane assessment by single-section trace analysis.”, Scripta Mater., 2001, 44, pp. 2789-2794 Morawiec A., “Orientations and Rotations: Computations in Crystallographic Textures.”, Springer, 2004. 2014-08-25 MERCIER David

Large number of dislocation slip and twinning systems. Crystal Plasticity of alpha-Titanium (hcp)  Slip systems Pyr. 2nd ord. <c+a> {𝟏𝟏 𝟐 𝟐} <𝟏𝟏 𝟐 𝟑> Basal <a> {𝟎𝟎𝟎𝟏} <𝟏𝟏 𝟐 𝟎> Prism. 1st ord. <a> {𝟏𝟎 𝟏 𝟎} < 𝟏𝟏 𝟐 𝟎 > Prism. 2nd ord. <a> {𝟏𝟏 𝟐 𝟎} < 𝟏 𝟏𝟎𝟎> Pyr. 1st ord. <a> {𝟏𝟎 𝟏 𝟏} < 𝟏𝟏 𝟐 𝟎 > Pyr. 1st ord. <c+a> {𝟏𝟎 𝟏 𝟏} <𝟏𝟏 𝟐 𝟑>  Twin systems Tensile twinning {𝟏𝟎 𝟏 𝟐} < 𝟏𝟎 𝟏 𝟏 > Tensile twinning {𝟏𝟏 𝟐 𝟏} < 𝟏𝟏 𝟐 𝟔 > Compr. twinning {𝟏𝟎 𝟏 𝟏} < 𝟏 𝟎𝟏𝟐> Compr. twinning {𝟏𝟏 𝟐 𝟐} < 𝟏𝟏 𝟐 𝟑 > Large number of dislocation slip and twinning systems. 2014-08-25 MERCIER David

Criteria to predict the slip transmission N factor (from Livingston & Chalmers)1 Livingston J.D . & Chalmers B., “Multiple slip in bicrystal deformation”, Acta Met. 1957,5, pp. 322-327. Luster J. & Morris M.A., “Compatibility of deformation in two-phase Ti-Al alloys: Dependence on microstructure and orientation relationships.”, Metallurgical and Materials Transactions A, 1995, 26(7), pp. 1745-1756. Marcinkowski M. J. & Tseng W. F., “Dislocation behavior at tilt boundaries of infinite extent.”, Metallurgical Transactions, 1970, 1(12), pp. 3397-3401. Bieler T. R. et al., “The role of heterogeneous deformation on damage nucleation at grain boundaries in single phase metals.”, International Journal of Plasticity, 2009, 25(9), pp. 1655-1683. m’ factor (from Luster & Morris)2 Outgoing slip Incoming slip Residual Burgers vector3 Outgoing slip Incoming slip Schmid Factor, resolved shear stress…4 2014-08-25 MERCIER David

Strain Transfer parameters implemented in the toolbox 2014-08-25 MERCIER David

Experiments Modeling Outline Acquisition of EBSD map of the sample Selection of interesting GB using the MATLAB Toolbox/GUI Spherical indentation close to the chosen GBs Measurement of the topography by AFM and of the lattice rotation by EBSD Inclination of GB measured by FIB or serial polishing 1st slip transmission analysis via the MATLAB Toolbox/GUI Creation of output files for CPFEM 3D CPFE modeling EBSD map Experiments AFM topography of a residual indent Cross sectional view of GB Modeling Slip transmission model using CPFEM results and the MATLAB Toolbox/GUI CPFEM displacement result after bicrystal indentation 2014-08-25 MERCIER David

Reconstructed Boundaries file EBSD on Ti–5Al–2.5Sn (wt%) sample Loading and Plot of EBSD data Outputs from OIM™ Data Analysis Grains number; Average orientation of each grains  Euler angles (phi1, PHI, phi2); Phase of material; Average positions and diameters of grains; GB numbers; GB trace coordinates ; Trace length and trace angle. Grain file type 2 and Reconstructed Boundaries file Loading of EBSD files. Setting of the coordinate system. Plot of the GBs segments. EBSD orientation map with IPF coloring scheme of Ti–5Al–2.5Sn (wt.%) sample. The sample exhibited a near-𝜶 (HCP) microstructure with the body centered cubic (BCC)  phase located primarily at α phase grain boundaries1.  Mean grain diameter : (34 ± 16)µm MATLAB Toolbox/GUI Seal J. R. et al., Mater. Sci. and Eng. A 552, 2012, pp. 61-68. 2014-08-25 MERCIER David

Introduction to the MATLAB toolbox 2014-08-25 MERCIER David

Selection of a specific grain boundary… Indentation experiments Gr. B GB Gr. B Gr. A Isolate a specific GB. Data transfer from EBSD map into a new window in order to analyze in detail the given bicrystal… AFM topography of residual indent in Ti-5Al-2.5Sn, close to a grain boundary with profiles of pile-up surrounding the indent. 2014-08-25 MERCIER David

CPFE model generation from the GUI Possibility to tune the indenter geometry (tip radius, apex angle…), sample geometry (GB inclination, sample size…), the mesh parameters (bias, number of elements…)… Generation of mesh procedure file and material config. file using Python scripts. 2014-08-25 MERCIER David

Few details about CPFE model Generation of a CPFE model with the MATLAB Toolbox/GUI Flow rule given by Kalidindi’s constitutive model1,2,3 Only Prismatic 1st order <a>, Basal <a> and Pyramidal 1st order <c+a> Gr. B Gr. A The CPFE model used is purely local formulation, and includes only the changes in slip system alignment across the boundary, but no strengthening effect from grain boundaries. DAMASK  http://damask.mpie.de/ References S.R. Kalidindi and L. Anand, “An approximate procedure for predicting the evolution of crystallographic texture in bulk deformtion processing of FFC metals.”, Int. J. Mech. Sci. 34(4) (1992) pp. 309-329. A.A. Salem et al., “Strain hardening due to deformation twinning in alpha-titanium: Constitutive relations and crystal-plasticity modeling.”, Acta Materialia 53(12) (2005) pp. 3495-3502. X. Wu et al., “Prediction of crystallographic texture evolution and anisotropic stress-strain curves during large plastic strains in high purity alpha-titanium using a taylor-type crystal plasticity model.”, Acta Materialia, 55(2) (2007) pp. 423-432J. Zambaldi C. et al. “Orientation informed nanoindentation of α-titanium: Indentation pileup in hexagonal metals deforming by prismatic slip.”, J. of Mater. Res., 2012, 27(01), pp. 356-367 2014-08-25 MERCIER David

Calculated topography from CPFEM of spherical indent close to a GB. CPFEM results (1/3) Gr. A Gr. B Gr. A Gr. B AFM topography of residual indent in Ti-5Al-2.5Sn, close to a grain boundary. To do this process many times…. (statistics…) Calculated topography from CPFEM of spherical indent close to a GB. Small discrepancy between experimental and simulated pile-up topographies indicate strain transfer is mainly controlled by geometrical consideration. 2014-08-25 MERCIER David

Local Misorientation from EBSD measurement vs CPFEM results. Gr. B Gr. A Gr. A Gr. B Local Misorientation from EBSD measurement vs CPFEM results. The CPFE model with no strengthening effect from grain boundaries seems to predict almost correctly the plasticity transfer. 2014-08-25 MERCIER David

CPFEM results (3/3) Accumulated prism. 1<a> shear Gr. A Accumulated basal shear Gr. B Isosurfaces of accumulated shear int the bicrystal obtained by CPFEM. Slip transfer is based on the geometrical compatibility of the two grains (high m’ value for prism. 1 <a> and basal, low RBV, high LRB…). 2014-08-25 MERCIER David

Fast transfer of experimental data into simulation input files : Advantages of the GUI Analysis of all GBs in a map (and color coded results), then selection of interesting ones Fast transfer of experimental data into simulation input files : SX indentation BX indentation Reduction of possible sources of error in analysis by visualization, standardized workflow and automated data I/O Readily extendible to other experiments : Polycrystal tensile test µ-cantilever bending test µ-pillar compression test Straining test and TEM Cu bi-crystal Straining test and TEM3. Zhao Z. et al., “Investigation of three-dimensional aspects of grain-scale plastic surface deformation of an aluminum oligocrystal.”, International Journal of Plasticity 24, 2008, pp. 2278-2297. Dehm G. et al., “Plasticity and Fracture at Small Length Scales: from Single Crystals towards Interfaces.”, Workshop on Mechanical Behaviour of Systems – 4, 2013 (India). Shen Z. et al., “Dislocation and grain boundary interactions in metal.”, Acta Metal., 1988, 36(12), pp. 3231-3242. Tensile test of Aluminum oligocrystal “dogbone”1. µ-pillar compression test and µ-cantilever bending test 2. 2014-08-25 MERCIER David

Results from in situ straining test in TEM (Kacher et al. 2012)  “In situ and tomographic analysis of dislocation/grain boundary interactions in a-titanium.”, Phil. Mag., 2014, pp. 1-16. Good agreement in term of residual Burgers vector calculated with the MATLAB Toolbox and values given in Kacher’s paper. 2014-08-25 MERCIER David

Results from polycrystal tensile test (Patriarca et al. 2014)  “Slip transmission in bcc FeCr polycrystal.”, Materials Science and Engineering: A, 2014, 588, pp. 308-317. Good agreement in term of residual Burgers vector calculated with the MATLAB Toolbox and values given in Patriarca’s paper. 2014-08-25 MERCIER David

Conclusion and Outlook MATLAB Toolbox / GUI = “Bridge between EBSD and CPFEM” For bcc, fcc and hcp materials and for 1 or 2 phase materials Slip trace analysis Many functions implemented to analyze and to quantify the potential for slip transmission at GBs Interfaced with Python code to rapidly generate CPFE simulation input files for indentation experiments Possibility to implement new functions and new CPFE models for other experiments (µ-cantilever, µ-pillar, straining test…) http://github.com/czambaldi/stabix Proceedings paper on ICOTOM17 conference Preliminary results : CPFE model with no strengthening effect from grain boundaries seems to predict almost correctly the plasticity transfer. More indentation and 3D EBSD experiments to do… 2014-08-25 MERCIER David

Thanks for your attention…. d.mercier@mpie.de Acknowledgments and Questions Dr. P. Eisenlohr, Dr. M. Crimp and Y. Su are acknowledged. Materials World Network grant references NSF: DFG: ZA523/3-1 Thanks for your attention…. Questions ? d.mercier@mpie.de 2014-08-25 MERCIER David