Rate-Controlling Microplastic Processes during Plastic Flow in FCC Metals: Origin of the Variation of Strain Rate Sensitivity in Aluminum from 78 to 300 K

The thermodynamic response of dislocation intersections with forest dislocations and other deformation products is recorded using the Eyring rate relation wherein the application of shear stress increases the probability of activation at a given strain rate and temperature. The inverse activation volume, 1/ν, can be directly determined by instantaneous strain-rate change and its dependence on flow stress, τ, defines the strain-rate sensitivity, S, through the Haasen plot slope. A linear slope over a large strain interval is observed even for a heterogeneous distribution of obstacles that could be of more than one type of obstacles encountered by the gliding dislocation. It was deduced that ν and τ at each activation site are coordinated by the internal stress resulting in constant activation work (k/S). The stress changes from down-rate changes become larger than that from up-rate changes due to the formation of weaker obstacles, resulting in a composite S, whereas only forest dislocations are detected by the up-change. The additivity of 1/ν was used to separate obstacle species in specially prepared AA1100 and super-pure aluminum from 78 to 300 K. The deduction that repulsive intersection is the rate-controlling process and creates vacancies at each intersection site depending on temperature was validated by observing the pinning and depinning of dislocations via pipe diffusion above 125 K. A new method to separate S for dislocation-dislocation intersections from the intersections with other obstacles and their temperature dependence is presented and validated.

[1]  M. Niewczas,et al.  Assimilated Model of Work-Hardening in FCC Metals and its Application to Devolution of Stored Work , 2022, Materials Today Communications.

[2]  B. Diak,et al.  Advanced method for structure-strength-ductility assessment of dispersion-strengthened FCC metals using activation work, mean slip distance and constitutive relation analyses: Decoding the Haasen plot , 2021, Materials Science and Engineering: A.

[3]  M. Niewczas,et al.  Forensic analyses of microstructure evolution of stage II & III: New assimilated model for work-hardening in FCC metals , 2020 .

[4]  S. Saimoto Deformation kinetics and constitutive relation analyses of bifurcation in work-hardening of face-centred cubic metals at cryogenic temperatures , 2019, Acta Materialia.

[5]  M. Niewczas,et al.  Specific resistivity of dislocations and vacancies for super-pure aluminium at 4.2 K determined in-situ and post-recovery deformation and correlated to flow stress , 2019, Philosophical Magazine A.

[6]  K. Matsuda,et al.  Muon Spin Relaxation Study of Solute–Vacancy Interactions During Natural Aging of Al-Mg-Si-Cu Alloys , 2019, Metallurgical and Materials Transactions A.

[7]  K. Inal,et al.  Small-angle X-ray scattering investigation of deformation-induced nanovoids in AA6063 aluminium alloy , 2017 .

[8]  Joshua C. Crone,et al.  Capturing the effects of free surfaces on void strengthening with dislocation dynamics , 2015 .

[9]  H. Wang,et al.  Interstitial loop strengthening upon deformation in aluminum via molecular dynamics simulations , 2013 .

[10]  D. Lloyd,et al.  A new analysis of yielding and work hardening in AA1100 and AA5754 at low temperatures , 2012 .

[11]  B. Diak,et al.  Point defect generation, nano-void formation and growth. I. Validation , 2012 .

[12]  D. Lloyd,et al.  Point defect generation, nano-void formation and growth. II. Criterion for ductile failure , 2012 .

[13]  A. Brahme,et al.  A new strain hardening model for rate-dependent crystal plasticity , 2011 .

[14]  H. Wang,et al.  The formation of stacking fault tetrahedra in Al and Cu: I. Dipole annihilation and the nucleation stage , 2011 .

[15]  P. Van Houtte,et al.  Constitutive relation based on Taylor slip analysis to replicate work-hardening evolution , 2011 .

[16]  S. Saimoto Detection of nano-particles by dynamic dislocation-defect analysis , 2010 .

[17]  R. Mishra,et al.  Recovery studies of cold rolled aluminum sheet using X-ray line broadening and activation volume determinations , 2009 .

[18]  H. Larsen,et al.  Kinetic analysis of dynamic point defect pinning in aluminium initiated by strain rate changes , 2009 .

[19]  M. Niewczas,et al.  Molecular dynamics studies of the interaction of a/6 ⟨112⟩ Shockley dislocations with stacking fault tetrahedra in copper. Part I: Intersection of SFT by an isolated Shockley , 2009 .

[20]  M. Niewczas,et al.  Plastic deformation of Al and AA5754 between 4.2 K and 295 K , 2008 .

[21]  S. Saimoto Dynamic manifestation of point defects on flow stress and the role of grain boundary as vacancy sinks , 2008 .

[22]  B. Diak,et al.  Dynamic Dislocation-Defect Analysis and SAXS Study of Nanovoid Formation in Aluminum Alloys , 2008 .

[23]  C. Wolverton Solute–vacancy binding in aluminum , 2007 .

[24]  S. Saimoto,et al.  Effects of Solubility Limit and the Presence of Ultra-Fine Al6Fe on the Kinetics of Grain Growth in Dilute Al-Fe Alloys , 2007 .

[25]  S. Saimoto Dynamic dislocation–defect analysis , 2006 .

[26]  Y. Bréchet,et al.  Atomic-scale study of dislocation glide in a model solid solution , 2006 .

[27]  D. Rodney,et al.  Atomic-scale study of dislocation–stacking fault tetrahedron interactions. Part I: mechanisms , 2006 .

[28]  H. Ogi,et al.  Acoustic study of kinetics of vacancy diffusion toward dislocations in aluminum , 2005 .

[29]  L. M. Brown,et al.  The enumeration and transformation of dislocation dipoles I. The dipole strengths of closed and open dislocation arrays , 2004 .

[30]  M. Kiritani,et al.  Cryo-transfer TEM study of vacancy cluster formation in thin films of aluminum and copper elongated at low temperature , 2003 .

[31]  G. Langelaan,et al.  Thermal expansion measurement of pure aluminum using a very low thermal expansion heating stage for x-ray diffraction experiments , 1999 .

[32]  B. Diak,et al.  Characterization of thermodynamic response by materials testing , 1998 .

[33]  F. Nabarro Cottrell-stokes law and activation theory , 1990 .

[34]  F. Brotzen,et al.  Diffusion near dislocations, dislocation arrays and tensile cracks , 1989 .

[35]  J. Martín,et al.  A study of cross-slip activation parameters in pure copper , 1988 .

[36]  R. Asaro,et al.  Overview no. 42 Texture development and strain hardening in rate dependent polycrystals , 1985 .

[37]  S. Saimoto,et al.  A re-examination of the cottrell-stokes relation based on precision measurements of the activation volume , 1983 .

[38]  S. Saimoto,et al.  Microplastic bases for constitutive relations found in tensile testing , 1981 .

[39]  Z. S. Basinski,et al.  Resistivity change with deformation of high purity Cu crystals and its subsequent recovery , 1977 .

[40]  J. Slakhorst,et al.  The Development of Rolling and Recrystallization Textures in High Purity Al , 1977, International Journal of Materials Research.

[41]  R. Balluffi Vacancy defect mobilities and binding energies obtained from annealing studies , 1976 .

[42]  C. Davies,et al.  Thermally activated dislocation intersection in face‐centered cubic metals , 1973 .

[43]  H. Fujita Continuous Observation of Dynamic Behaviors of Dislocations in Aluminum , 1967 .

[44]  J. Lothe,et al.  GLIDE OF JOGGED DISLOCATIONS , 1967 .

[45]  Z. S. Basinski,et al.  RESISTIVITY OF DEFORMED CRYSTALS , 1967 .

[46]  M. Makin,et al.  DISLOCATION MOVEMENT THROUGH RANDOM ARRAYS OF OBSTACLES , 1966 .

[47]  P. Hirsch Extended jogs in dislocations in face-centred cubic metals , 1962 .

[48]  Z. S. Basinski Thermally activated glide in face-centred cubic metals and its application to the theory of strain hardening , 1959 .

[49]  M. Makin The temperature dependence of flow stress in copper single crystals , 1958 .

[50]  A. Cottrell,et al.  Effects of temperature on the plastic properties of aluminium crystals , 1955, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[51]  A. Cottrell,et al.  CXXXI. Effect of temperature on the flow stress of work-hardened copper crystals , 1955 .

[52]  J. E. Dorn,et al.  The Effect of Thermal-Mechanical History on the Strain Hardening of Metals, , 1948 .