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Methodology
Micromechanical Deformation of Two-Phase Ti Alloys, Informed by EBSD Characterisation
Tea-Sung (Terry) Jun*, Giorgio Sernicola, Vivian Tong, Fionn P E Dunne, T Ben Britton
Department of Materials, Imperial College of London, Exhibition Road, London, SW7 2AZ, UK
Motivation
Results
Key findings Acknowledgement
● Cold dwell fatigue has been a long-standing issue in aero-engine industry.
● Dwell susceptible alloys are those which suffer from a reduction in the life due to
the inclusion of a short load-hold (~120s) in fatigue.
● This could be either be a chemical, structural or morphological effect due to
difference in β-phase volume fraction and local chemistry.
● As dwell includes a time-dependant holding step, rate sensitivity and the
resultant load shedding are clearly crucial factors in the dwell phenomenon.
Ti-6Al-2Sn-4Zr-2Mo(dwell sensitive) Ti-6Al-2Sn-4Zr-6Mo(not dwell sensitive)
EBSD orientation maps observed with respect to normal to the forging direction
Aims
● To develop a methodology for investigating micromechanics of two-phase materials
● To study a local deformation mechanism of two-phase Ti624x (x=2 and 6 Mo)
● To understand the effect of α/β morphology on σ-ε behaviour
● To measure micromechanical rate sensitivity
(left) ‘Rogue’ grain combination and (right) the resultant stress variation along the path A-A′ [1]
1. Material processing
○ Create large α-lamellar separated by thin β-
ligaments, to make micropillars of α-β-α structure
2. EBSD mapping (Bruker)
3. Regions of Interests (ROIs)
4. FIB – micropillar fabrication 5. SEM/Alemnis in-situ compression
front back side1 side2
○ Square pillar: easy slip trace analysis, In-situ HR-EBSD
○ Find comparable grains between Ti6242&6 by comparing misorientation and Schmid factor(M)
Large EBSD map of α phase β-reconstruction [2] Smaller EBSD map of α/β phase
and
EBSD Characterisation
We are grateful to the Engineering and Physical Science
Research Council for funding through HexMat (EP/K034332/1).
Contact
▪ Email: t.jun@imperial.ac.uk (or terryjun83@gmail.com)
▪ http://www3.imperial.ac.uk/engineeringalloys
▪ http://www3.imperial.ac.uk/hexmat
Morphology Effects
Local Deformation Behaviour Rate Sensitivity
Ti6242 Ti6246
○ Pillars from Ti6242-A1: same α orientation, same strain rate (1.2x10-3s-1), various β morphology
○ Pillar details: a top width of 2µm, an aspect ratio of 1.9:1~2.2:1 and taper angle of ~5.5°
Similar β morphology
Different β morphology
Slip System Primary slip Mode SF(A2) SF(B2)
Basal
(0001)<11-20>
B1 0.101 0.087
B2 0.461 0.432
B3 0.361 0.345
Prismatic
{10-10}<11-20>
P1 0.188 0.147
P2 0.111 0.091
P3 0.077 0.056
Slip System Primary slip Mode SF(A3) SF(B3)
Basal
(0001)<11-20>
B1 0.068 0.052
B2 0.023 0.019
B3 0.046 0.033
Prismatic
{10-10}<11-20>
P1 0.493 0.488
P2 0.306 0.334
P3 0.186 0.154
Schmid Factors (A2 & B2) Schmid Factors (A3 & B3)
α[197,20,157]
β[296,36,30]
A1
8µm
30µm 30µm 30µm
30µm
α[20,38,318]
β[302,37,30]
α[125,86,229]
β[229,19,121]
α[117,87,231]
Β[249,4,92]
α[19,33,319]
Β[149,17,217]
A2
A3
B3 B2
300µm
Strain Rate Sensitivity exponent:Basal slip
Prism slip
Side2view
Front view
Loading Ti6242-A2
Side2
Ti6246-B2
Side2
Ti6242-A3 Ti6246-B3
Front Front
Slip trace analysis on deformed pillars: yellow and blue arrows indicate primary
and secondary slip system, respectively, anticipated from Schmid factor calculation
σ-ε responseB
P
B B
P P
● Combination of EBSD, FIB and Nanoindenter is an effective tool to investigate micromechanical deformation of two-phase materials.
● EBSD was effectively used to select individual slip systems.
● Both Ti6242 and Ti6246 are rate-sensitive : Ti6242 as a slip system dependent and Ti6246 as a slip system independent rate sensitive.
Engineering Stress vs. Engineering Strain in Ti6242(A2,A3) and Ti6246(B2,B3)
 Experiments: displacement control, strain rates of 1.5x10-4s-1 ~ 1.0x10-2s-1
Large EBSD maps on Ti6242 and Ti6246, including smaller maps of ROIs: A1 for morphology study and A2-B2 & A3-B3 have comparable α crystal structure
200µm 60µm
Experimental setup of pillar compression using 10µm dia. flat punch tip
Micropillar fabricated using Helios Nanolab focused ion
beam (FIB) with an aid of a script created by AutoScriptTM
▪ Similar β morphology, similar σ-ε response in elastic and early stage of plastic regime
▪ Schmid’s law works well to anticipate local deformation behaviour ▪ Quite different σ-ε responses in basal/prism slip in Ti6242, but similar in Ti6246
B B
P P
Strain Rate (έ) vs. Flow Stress (at ε=0.5) in log-log form
▪ Ti6242: different m values with respect to activated slip system
▪ Ti6246: similar m values regardless of activated slip system
References [1] D.L. McDowell and F.P.E. Dunne (2010) Int J Fatigue, [2] Courtesy of Prof. Bradley P Wynne (Univ. of Sheffield)
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EBSD Conference_Terry

  • 1. Methodology Micromechanical Deformation of Two-Phase Ti Alloys, Informed by EBSD Characterisation Tea-Sung (Terry) Jun*, Giorgio Sernicola, Vivian Tong, Fionn P E Dunne, T Ben Britton Department of Materials, Imperial College of London, Exhibition Road, London, SW7 2AZ, UK Motivation Results Key findings Acknowledgement ● Cold dwell fatigue has been a long-standing issue in aero-engine industry. ● Dwell susceptible alloys are those which suffer from a reduction in the life due to the inclusion of a short load-hold (~120s) in fatigue. ● This could be either be a chemical, structural or morphological effect due to difference in β-phase volume fraction and local chemistry. ● As dwell includes a time-dependant holding step, rate sensitivity and the resultant load shedding are clearly crucial factors in the dwell phenomenon. Ti-6Al-2Sn-4Zr-2Mo(dwell sensitive) Ti-6Al-2Sn-4Zr-6Mo(not dwell sensitive) EBSD orientation maps observed with respect to normal to the forging direction Aims ● To develop a methodology for investigating micromechanics of two-phase materials ● To study a local deformation mechanism of two-phase Ti624x (x=2 and 6 Mo) ● To understand the effect of α/β morphology on σ-ε behaviour ● To measure micromechanical rate sensitivity (left) ‘Rogue’ grain combination and (right) the resultant stress variation along the path A-A′ [1] 1. Material processing ○ Create large α-lamellar separated by thin β- ligaments, to make micropillars of α-β-α structure 2. EBSD mapping (Bruker) 3. Regions of Interests (ROIs) 4. FIB – micropillar fabrication 5. SEM/Alemnis in-situ compression front back side1 side2 ○ Square pillar: easy slip trace analysis, In-situ HR-EBSD ○ Find comparable grains between Ti6242&6 by comparing misorientation and Schmid factor(M) Large EBSD map of α phase β-reconstruction [2] Smaller EBSD map of α/β phase and EBSD Characterisation We are grateful to the Engineering and Physical Science Research Council for funding through HexMat (EP/K034332/1). Contact ▪ Email: t.jun@imperial.ac.uk (or terryjun83@gmail.com) ▪ http://www3.imperial.ac.uk/engineeringalloys ▪ http://www3.imperial.ac.uk/hexmat Morphology Effects Local Deformation Behaviour Rate Sensitivity Ti6242 Ti6246 ○ Pillars from Ti6242-A1: same α orientation, same strain rate (1.2x10-3s-1), various β morphology ○ Pillar details: a top width of 2µm, an aspect ratio of 1.9:1~2.2:1 and taper angle of ~5.5° Similar β morphology Different β morphology Slip System Primary slip Mode SF(A2) SF(B2) Basal (0001)<11-20> B1 0.101 0.087 B2 0.461 0.432 B3 0.361 0.345 Prismatic {10-10}<11-20> P1 0.188 0.147 P2 0.111 0.091 P3 0.077 0.056 Slip System Primary slip Mode SF(A3) SF(B3) Basal (0001)<11-20> B1 0.068 0.052 B2 0.023 0.019 B3 0.046 0.033 Prismatic {10-10}<11-20> P1 0.493 0.488 P2 0.306 0.334 P3 0.186 0.154 Schmid Factors (A2 & B2) Schmid Factors (A3 & B3) α[197,20,157] β[296,36,30] A1 8µm 30µm 30µm 30µm 30µm α[20,38,318] β[302,37,30] α[125,86,229] β[229,19,121] α[117,87,231] Β[249,4,92] α[19,33,319] Β[149,17,217] A2 A3 B3 B2 300µm Strain Rate Sensitivity exponent:Basal slip Prism slip Side2view Front view Loading Ti6242-A2 Side2 Ti6246-B2 Side2 Ti6242-A3 Ti6246-B3 Front Front Slip trace analysis on deformed pillars: yellow and blue arrows indicate primary and secondary slip system, respectively, anticipated from Schmid factor calculation σ-ε responseB P B B P P ● Combination of EBSD, FIB and Nanoindenter is an effective tool to investigate micromechanical deformation of two-phase materials. ● EBSD was effectively used to select individual slip systems. ● Both Ti6242 and Ti6246 are rate-sensitive : Ti6242 as a slip system dependent and Ti6246 as a slip system independent rate sensitive. Engineering Stress vs. Engineering Strain in Ti6242(A2,A3) and Ti6246(B2,B3)  Experiments: displacement control, strain rates of 1.5x10-4s-1 ~ 1.0x10-2s-1 Large EBSD maps on Ti6242 and Ti6246, including smaller maps of ROIs: A1 for morphology study and A2-B2 & A3-B3 have comparable α crystal structure 200µm 60µm Experimental setup of pillar compression using 10µm dia. flat punch tip Micropillar fabricated using Helios Nanolab focused ion beam (FIB) with an aid of a script created by AutoScriptTM ▪ Similar β morphology, similar σ-ε response in elastic and early stage of plastic regime ▪ Schmid’s law works well to anticipate local deformation behaviour ▪ Quite different σ-ε responses in basal/prism slip in Ti6242, but similar in Ti6246 B B P P Strain Rate (έ) vs. Flow Stress (at ε=0.5) in log-log form ▪ Ti6242: different m values with respect to activated slip system ▪ Ti6246: similar m values regardless of activated slip system References [1] D.L. McDowell and F.P.E. Dunne (2010) Int J Fatigue, [2] Courtesy of Prof. Bradley P Wynne (Univ. of Sheffield) Load