• Keine Ergebnisse gefunden

4.2 Recrystallization mechanisms of Mg-Nd based alloys

4.2.3 Strain induced grain boundary migration

Twins play an important role in recrystallization behaviors because twins are severely deformed and have high stored energy. In addition, grain boundaries also hinder the dislocation movement, and they are the potential sites for recrystallization. However, there are very few recrystallized grains found at the grain boundary regions in the present quasi in-situ experiments. Nevertheless, the strain induced grain boundary migration is observed in the AN12 sample, as shown in Figure. 4.2.5. After the annealing at 400 °C for 1 min, the boundaries of the grains A and B move towards the twins of neighboring grain, forming a dislocation-free region marked with the white arrows in Figure. 4.2.5 (b). The misorientations between these regions and grain A or B are lower than 10° as no HAGBs are observed. Rather than regarding the marked

79

regions as newly formed recrystallized grains, it is more reasonable to relate them with grain boundary migration. These regions can continuously grow by consuming other twins with annealing time, as shown in Figure. 4.2.5 (c). TKD observation of the same sample also supports the mechanism, Figure. 4.2.5 (d).

The grain C stabs into the grain D. The grain boundary between C and D has a very high curvature that seems to be uncommon. The assumption makes sense that the grain boundary from its original place marked with the white dash line move towards grain D by consuming the twin band. The grain boundary migration is preferred at the junctions of twin and grain boundary. Compared with normal grain boundaries, the junctions of twin and grain boundary have a higher dislocation density and stored energy because of twinning. The dislocation and energy localization at the junctions can be released by grain boundary migration that forms the low dislocation region.

Figure. 4.2.5 EBSD maps of quasi in-situ AN12 sample: (a) as-rolled, (b) annealed at 270 °C for 1 min and (c) annealed at 270 °C for 3 min, (d) IPF map of the AN12 TKD sample annealed at 270 °C for 1 min.

Various mechanisms are considered to comprehend the recrystallization behaviors of the AN12 and ZN12 samples. The recrystallization processes of both samples, based on the present experimental results, are schematically illustrated in Figure. 4.2.6. Twins are observed in the as-rolled AN12 and ZN12 samples.

Secondary twins are dominant in the AN12 sample, Figure. 4.2.6 (a). Other types of twins, e.g., ternary twin, play an important role in the ZN12 sample. During recrystallization annealing, small nuclei are formed inside the secondary twin of the grain A. These nuclei inherit the orientation of the secondary twins having the RD split of basal poles, and they grow rapidly along the twins, as shown in Figure. 4.2.6 (c). Besides, the grain boundaries of grain C migrate towards the twin in grain B because of a high stored energy and dislocation density. It helps strengthen the deformation basal texture as some deformed grains are becoming larger. On the contrary, some small precipitates are formed at the grain and twin boundaries in the ZN12

80

sample. These precipitates pin the boundaries and retard the recrystallization process. Recovery accompanying the formation of dislocation cells is pronounced in the ZN12 sample. It is difficult for the dislocation cells to merge and form large recrystallized grains because the LAGBs can also be pinned by precipitates or segregation of Zn and RE. The preferential growth of RD split nucleus inside secondary twins is restricted by precipitation. As a result, the texture of recrystallized grains becomes more scattered in ZN12 sample than AN12 sample.

Figure. 4.2.6 Schematic of recrystallization mechanisms in: (a) and (c) the AN12 sample, (b) and (d) the ZN12 sample.

81

5 Summary

The understanding of the deformation and recrystallization mechanisms of Mg-RE alloys is of importance to develop high performance Mg alloys. To reach these complicated goals, quasi in-situ tensile and recrystallization annealing experiments were applied in this study. Distinct differences in the yielding, fracture behaviors and strain hardening are observed during the quasi in-situ tension. The slip traces and active twin variants reveal the contributions of different deformation modes to accommodate the strain during uniaxial tension.

1. The ZN12 sample shows a lower yield strength and higher elongation than the AN12 in conventional tensile tests. An obvious yielding is observed in the ZN12 sample. It is related to the formation of twins which releases the local stress. The calculated strain hardening rate exhibits a higher strain hardening exponent of the ZN12 than that of the AN12 sample.

2. Basal slip is the dominant deformation mode in quasi in-situ tensile tests. Most of the grains already show obvious basal slip traces after the yielding in the ZN12 sample, indicating a homogeneous deformation.

Meanwhile, some non-basal slip traces are also observed in the grain boundary region of the ZN12 sample.

The slip traces become wavy with increasing the strain. On the contrary, basal slip traces are rarely found in the AN12 sample at ε = 0.02. Even at ε = 0.08, the basal slip traces are localized in limited number of grains.

3. Apart from basal slip, tensile twinning plays a role in accommodating the strain. The number of the twins in the AN12 and ZN12 samples at ε = 0.08 are 255 and 147, respectively. It is of interest to find that half of the twins in the ZN12 sample are already found at ε = 0.02 while most of the twins in the AN12 sample are formed at ε = 0.08. Tensile twinning reorients the basal poles of the matrix grains from the ND to TD, i.e., the basal-type to TD spread orientation. With increasing strain, more twins are formed, and the twins formed at low strain gradually grow at the same time. As a result, the texture component corresponding to the TD spread in basal pole figure becomes sharper.

4. To minimize the effects of grain size and initial texture on the quasi in-situ tensile experiments, the EBSD data are carefully evaluated. The grains are categorized into several subsets based on the grain size and SF.

Thus, the grains in the same subsets can be compared between the AN12 and ZN12 samples without concerning the influence of grain size and orientation. There still remains an obvious trend that non-basal slip and tensile twinning are more preferred in ZN12 than AN12 sample, especially at low strain.

5. The chemical composition is one of the main factors that induced the distinct mechanical properties in the AN12 and ZN12. It results in a lower CRSS for basal slip and a lower CRSS ratio of non-basal to basal slip in the ZN12 compared with the AN12 sample.

82

Recrystallization annealing is used to modify the microstructure and texture after the thermomechanical processing. The addition of RE into Mg alloys was reported to alter the recrystallization mechanisms of Mg alloys and produce the so-called RE texture. Obvious differences in the recrystallization kinetics, nucleation and grain growth process are observed between the AN12 and ZN12 during quasi in-situ annealing.

1. The AN12 sample has higher recrystallization kinetics than the ZN12 sample. Fully recrystallization is achieved in the AN12 after 18 min annealing at 350 °C, while the recrystallization is negligible in the ZN12 sample with the same annealing parameter. Due to the significant difference in recrystallization kinetics, quasi in-situ annealing at 270 °C and 400 °C are applied to the AN12 and ZN12, respectively.

2. Secondary twinning is the dominant twinning mode in the as-rolled sample. Secondary twins are the preferred sites for nucleation in the AN12 sample. The c-axis of recrystallization nuclei of both alloys are tilted from ND to RD, similar to the secondary twin orientation. In addition, the secondary twins in the ZN12 sample have a wider spread towards TD compared with those in the AN12 sample.

3. Obvious precipitation at twin and grain boundaries is observed in the ZN12 sample. It is responsible for the retarded recrystallization. In the early stage of annealing, the dislocation cells as an indicator of recovery are formed in the ZN12 sample, which reduces the stored energy. On the contrary, the AN12 sample with clear boundaries and a high dislocation density promotes the twin induced nucleation mechanisms.

4. The growth preference is evaluated by tracing the diameter of recrystallized grains. In the AN12 sample, the growing grains (g ≥ 0.2) showed the RD split orientations which are responsible for the texture of recrystallized grains with a wide spread of the basal pole from the ND to RD. However, the newly formed grains (g = ∞) other than the growing ones are the majority of the recrystallized grains after 8 min annealing in the ZN12 sample. They showed a weak and scattered orientations in the (0001) pole figure.

To conclude, the ZN12 sample shows better formability than the AN12 sample, owing to the easier activation of different deformation modes. Apart from the effect of grain size and texture, the chemical composition by changing the CRSS value is important to explain the multiple dislocation slip and twinning activities in the ZN12 sample. During annealing, the recrystallization in the ZN12 sample is retarded by the segregation and precipitation at the twin boundaries. The complex twinning behaviors in the ZN12 sample result in a wide spread orientation of the recrystallized nuclei. The recrystallized grain originating from secondary twins in the AN12 sample can easily grow which inherit the RD spread texture of secondary twins.

83

Reference

[1] S. Schumann, H. Friedrich, Current and future use of magnesium in the automobile industry, Materials Science Forum (2003) Medium: X; Size: page(s) 51-56.

[2] K.U. Kainer, F. von Buch, The Current State of Technology and Potential for Further Development of Magnesium Applications, Magnesium – Alloys and Technology, pp. 1-22.

[3] F. Witte, N. Hort, C. Vogt, S. Cohen, K.U. Kainer, R. Willumeit, F. Feyerabend, Degradable biomaterials based on magnesium corrosion, Current Opinion in Solid State and Materials Science 12(5) (2008) 63-72.

[4] B.L. Mordike, T. Ebert, Magnesium: Properties — applications — potential, Materials Science and Engineering: A 302(1) (2001) 37-45.

[5] R.W. Cahn, Binary Alloy Phase Diagrams–Second edition. T. B. Massalski, Editor-in-Chief; H.

Okamoto, P. R. Subramanian, L. Kacprzak, Editors. ASM International, Materials Park, Ohio, USA.

December 1990. xxii, 3589 pp., Advanced Materials 3(12) (1991) 628-629.

[6] S.R. Agnew, J.A. Horton, M.H. Yoo, Transmission electron microscopy investigation of 〈c+a〉

dislocations in Mg and α-solid solution Mg-Li alloys, Metallurgical and Materials Transactions A 33(3) (2002) 851-858.

[7] F. Hollrigl-Rosta, E. Just, J. Kohler, H.J. Melzer, MAGNESIUM IN THE VOLKSWAGEN, Light Metal Age 38(7-8) (1980) 22-23, 26-28.

[8] L.L. Rokhlin, Magnesium Alloys Containning Rare Earth Metals, Taylor & Francis, London, 2003.

[9] S. Yi, J. Bohlen, F. Heinemann, D. Letzig, Mechanical anisotropy and deep drawing behaviour of AZ31 and ZE10 magnesium alloy sheets, Acta Materialia 58(2) (2010) 592-605.

[10] U.F. Kocks, H.-R. Wenk, C.N. Tomé, Texture and anisotropy : preferred orientations in polycrystals and their effect on materials properties, Cambridge University Press, Cambridge, 1998.

[11] T. Obara, H. Yoshinga, S. Morozumi, {112̄2}〈1123〉 Slip system in magnesium, Acta Metallurgica 21(7) (1973) 845-853.

[12] R.V. Mises, Mechanik der plastischen Formänderung von Kristallen, ZAMM - Journal of Applied Mathematics and Mechanics / Zeitschrift für Angewandte Mathematik und Mechanik 8(3) (1928) 161-185.

[13] Y. Chino, K. Sassa, A. Kamiya, M. Mabuchi, Stretch formability at elevated temperature of a cross-rolled AZ31 Mg alloy sheet with different rolling routes, Materials Science and Engineering: A 473(1) (2008) 195-200.

[14] J.-H. Cho, H.-W. Kim, S.-B. Kang, T.-S. Han, Bending behavior, and evolution of texture and microstructure during differential speed warm rolling of AZ31B magnesium alloys, Acta Materialia 59(14) (2011) 5638-5651.

[15] F. Basson, D. Letzig, Aluminium twin roll casting transfers benefits to magnesium, Aluminium International Today 22(6) (2010) 19.

84

[16] J. Bohlen, M.R. Nürnberg, J.W. Senn, D. Letzig, S.R. Agnew, The texture and anisotropy of magnesium–zinc–rare earth alloy sheets, Acta Materialia 55(6) (2007) 2101-2112.

[17] J. Bohlen, S. Yi, D. Letzig, K.U. Kainer, Effect of rare earth elements on the microstructure and texture development in magnesium–manganese alloys during extrusion, Materials Science and Engineering: A 527(26) (2010) 7092-7098.

[18] G.V. Raynor, The physical metallurgy of magnesium and its alloys, Pergamon1959.

[19] F. Hauser, Deformation and Fracture of Alpha Solid Solutions of Li in Mg, ASM, 1958.

[20] P.W. Flynn, Prismatic slip in magnesium single crystals, University of California, Berkeley1961.

[21] A.A. Nayeb-Hashemi, J.B. Clark, A.S.M. International, Phase diagrams of binary magnesium alloys, ASM International, Metals Park, Ohio, 1988.

[22] F.E. Hauser, P.R. Landon, J.E. Dorn, Deformation and Fracture of Alpha Solid Solutions of Lithium in Magnesium., 1958, pp. 856–883.

[23] P.W. Flynn, Prismatic slip in magnesium single crystals, University of California, Berkeley1961.

[24] K. Máthis, K. Nyilas, A. Axt, I. Dragomir-Cernatescu, T. Ungár, P. Lukáč, The evolution of non-basal dislocations as a function of deformation temperature in pure magnesium determined by X-ray diffraction, Acta Materialia 52(10) (2004) 2889-2894.

[25] S.R. Agnew, Ö. Duygulu, Plastic anisotropy and the role of non-basal slip in magnesium alloy AZ31B, International Journal of Plasticity 21(6) (2005) 1161-1193.

[26] M.R. Barnett, A taylor model based description of the proof stress of magnesium AZ31 during hot working, Metallurgical and Materials Transactions A 34(9) (2003) 1799-1806.

[27] M. Suzuki, H. Sato, K. Maruyama, H. Oikawa, Creep behavior and deformation microstructures of Mg–Y alloys at 550 K, Materials Science and Engineering: A 252(2) (1998) 248-255.

[28] S.R. Agnew, M.H. Yoo, C.N. Tomé, Application of texture simulation to understanding mechanical behavior of Mg and solid solution alloys containing Li or Y, Acta Materialia 49(20) (2001) 4277-4289.

[29] J.A. Yasi, L.G. Hector, D.R. Trinkle, Prediction of thermal cross-slip stress in magnesium alloys from direct first-principles data, Acta Materialia 59(14) (2011) 5652-5660.

[30] J.F. Nie, Effects of precipitate shape and orientation on dispersion strengthening in magnesium alloys, Scripta Materialia 48(8) (2003) 1009-1015.

[31] M.R. Barnett, Z. Keshavarz, A.G. Beer, D. Atwell, Influence of grain size on the compressive deformation of wrought Mg–3Al–1Zn, Acta Materialia 52(17) (2004) 5093-5103.

[32] J. Koike, New Deformation Mechanisms in Fine-Grain Mg Alloys, Materials Science Forum 419-422 (2003) 189-194.

[33] A. Jain, O. Duygulu, D.W. Brown, C.N. Tomé, S.R. Agnew, Grain size effects on the tensile properties and deformation mechanisms of a magnesium alloy, AZ31B, sheet, Materials Science and Engineering: A 486(1) (2008) 545-555.

85

[34] A. Couret, D. Caillard, An in situ study of prismatic glide in magnesium—I. The rate controlling mechanism, Acta Metallurgica 33(8) (1985) 1447-1454.

[35] H. Yoshinaga, R. Horiuchi, On the Nonbasal Slip in Magnesium Crystals, Transactions of the Japan Institute of Metals 5(1) (1964) 14-21.

[36] J. Wang, J.M. Molina-Aldareguía, J. Llorca, Effect of Al content on the critical resolved shear stress for twin nucleation and growth in Mg alloys, Acta Materialia 188 (2020) 215-227.

[37] M.R. Barnett, 3 - Twinning and its role in wrought magnesium alloys, in: C. Bettles, M. Barnett (Eds.), Advances in Wrought Magnesium Alloys, Woodhead Publishing2012, pp. 105-143.

[38] C.S. Roberts, Magnesium and its Alloys, Wiley1960.

[39] J. Wang, J.P. Hirth, C.N. Tomé, (1¯012) Twinning nucleation mechanisms in hexagonal-close-packed crystals, Acta Materialia 57(18) (2009) 5521-5530.

[40] L. Capolungo, I.J. Beyerlein, Nucleation and stability of twins in hcp metals, Physical Review B 78(2) (2008) 024117.

[41] I.J. Beyerlein, R.J. McCabe, C.N. Tomé, Effect of microstructure on the nucleation of deformation twins in polycrystalline high-purity magnesium: A multi-scale modeling study, Journal of the Mechanics and Physics of Solids 59(5) (2011) 988-1003.

[42] J.W. Christian, CHAPTER 2 - Formal Geometry of Crystal Lattices, in: J.W. Christian (Ed.), The Theory of Transformations in Metals and Alloys, Pergamon, Oxford, 2002, p. 48.

[43] A. Serra, D.J. Bacon, A new model for {1012} twin growth in hcp metals, Philosophical Magazine A 73(2) (1996) 333-343.

[44] F. Wang, C.D. Barrett, R.J. McCabe, H. El Kadiri, L. Capolungo, S.R. Agnew, Dislocation induced twin growth and formation of basal stacking faults in {101¯2} twins in pure Mg, Acta Materialia 165 (2019) 471-485.

[45] C. Cáceres, P. Lukáč, A. Blake, Strain hardening due to {10 1 2} twinning in pure magnesium, Philosophical Magazine 88(7) (2008) 991-1003.

[46] D.W. Brown, S.R. Agnew, M.A.M. Bourke, T.M. Holden, S.C. Vogel, C.N. Tomé, Internal strain and texture evolution during deformation twinning in magnesium, Materials Science and Engineering: A 399(1) (2005) 1-12.

[47] L. Jiang, J.J. Jonas, A.A. Luo, A.K. Sachdev, S. Godet, Twinning-induced softening in polycrystalline AM30 Mg alloy at moderate temperatures, Scripta Materialia 54(5) (2006) 771-775.

[48] I.J. Beyerlein, L. Capolungo, P.E. Marshall, R.J. McCabe, C.N. Tomé, Statistical analyses of deformation twinning in magnesium, Philosophical Magazine 90(16) (2010) 2161-2190.

[49] J.J. Jonas, S. Mu, T. Al-Samman, G. Gottstein, L. Jiang, Ė. Martin, The role of strain accommodation during the variant selection of primary twins in magnesium, Acta Materialia 59(5) (2011) 2046-2056.

86

[50] D. Guan, B. Wynne, J. Gao, Y. Huang, W.M. Rainforth, Basal slip mediated tension twin variant selection in magnesium WE43 alloy, Acta Materialia 170 (2019) 1-14.

[51] E. Kelley, W. Hosford, Plane-strain compression of magnesium and magnesium alloy crystals, Trans Met Soc AIME 242(1) (1968) 5-13.

[52] B.C. Wonsiewicz, W.A. Backofen, Plasticity of Magnesium Crystals, Trans Met Soc AIME 239(9) (1967) 1422-1433.

[53] A. Chapuis, J.H. Driver, Temperature dependency of slip and twinning in plane strain compressed magnesium single crystals, Acta Materialia 59(5) (2011) 1986-1994.

[54] M.A. Gharghouri, G.C. Weatherly, J.D. Embury, J. Root, Study of the mechanical properties of Mg-7.7at.% Al by in-situ neutron diffraction, Philosophical Magazine A 79(7) (1999) 1671-1695.

[55] A. Staroselsky, L. Anand, A constitutive model for hcp materials deforming by slip and twinning:

application to magnesium alloy AZ31B, International Journal of Plasticity 19(10) (2003) 1843-1864.

[56] S.R. Agnew, C.N. Tomé, D.W. Brown, T.M. Holden, S.C. Vogel, Study of slip mechanisms in a magnesium alloy by neutron diffraction and modeling, Scripta Materialia 48(8) (2003) 1003-1008.

[57] M.R. Barnett, Z. Keshavarz, X. Ma, A semianalytical sachs model for the flow stress of a magnesium alloy, Metallurgical and Materials Transactions A 37(7) (2006) 2283-2293.

[58] H. Yoshinaga, R. Horiuchi, Deformation Mechanisms in Magnesium Single Crystals Compressed in the Direction Parallel to Hexagonal Axis, Transactions of the Japan Institute of Metals 4(1) (1963) 1-8.

[59] W.B. Hutchinson, M.R. Barnett, Effective values of critical resolved shear stress for slip in polycrystalline magnesium and other hcp metals, Scripta Materialia 63(7) (2010) 737-740.

[60] J.F. Nie, Y.M. Zhu, J.Z. Liu, X.Y. Fang, Periodic Segregation of Solute Atoms in Fully Coherent Twin Boundaries, Science 340(6135) (2013) 957.

[61] J.B. Clark, Transmission electron microscopy study of age hardening in a Mg-5 wt.% Zn alloy, Acta Metallurgica 13(12) (1965) 1281-1289.

[62] N. Stanford, M.R. Barnett, Effect of particles on the formation of deformation twins in a magnesium-based alloy, Materials Science and Engineering: A 516(1) (2009) 226-234.

[63] M.A. Gharghouri, G.C. Weatherly, J.D. Embury, The interaction of twins and precipitates in a Mg-7.7 at.% Al alloy, Philosophical Magazine A 78(5) (1998) 1137-1149.

[64] J.D. Robson, N. Stanford, M.R. Barnett, Effect of precipitate shape on slip and twinning in magnesium alloys, Acta Materialia 59(5) (2011) 1945-1956.

[65] J.W. Christian, S. Mahajan, Deformation twinning, Progress in Materials Science 39(1) (1995) 86-87.

[66] M.R. Barnett, Twinning and the ductility of magnesium alloys: Part II. “Contraction” twins, Materials Science and Engineering: A 464(1) (2007) 8-16.

[67] M.A. Meyers, O. Vöhringer, V.A. Lubarda, The onset of twinning in metals: a constitutive description, Acta Materialia 49(19) (2001) 4025-4039.

87

[68] E. Schmid, W. Boas, Kristallplastizität (1935), Berlin. J. Springer.

[69] J.R. Luo, A. Godfrey, W. Liu, Q. Liu, Twinning behavior of a strongly basal textured AZ31 Mg alloy during warm rolling, Acta Materialia 60(5) (2012) 1986-1998.

[70] S. Sandlöbes, S. Zaefferer, I. Schestakow, S. Yi, R. Gonzalez-Martinez, On the role of non-basal deformation mechanisms for the ductility of Mg and Mg–Y alloys, Acta Materialia 59(2) (2011) 429-439.

[71] S. Mu, T. Al-Samman, V. Mohles, G. Gottstein, Cluster type grain interaction model including twinning for texture prediction: Application to magnesium alloys, Acta Materialia 59(18) (2011) 6938-6948.

[72] X. Li, T. Al-Samman, S. Mu, G. Gottstein, Texture and microstructure development during hot deformation of ME20 magnesium alloy: Experiments and simulations, Materials Science and Engineering:

A 528(27) (2011) 7915-7925.

[73] M.R. Barnett, M.D. Nave, C.J. Bettles, Deformation microstructures and textures of some cold rolled Mg alloys, Materials Science and Engineering: A 386(1) (2004) 205-211.

[74] J. Weertman, Steady‐State Creep through Dislocation Climb, Journal of Applied Physics 28(3) (1957) 362-364.

[75] H. Jazaeri, F.J. Humphreys, The transition from discontinuous to continuous recrystallization in some aluminium alloys: II – annealing behaviour, Acta Materialia 52(11) (2004) 3251-3262.

[76] F.J. Humphreys, M. Hatherly, Recrystallization and Related Annealing Phenomena, Elsevier, Oxford, 2004.

[77] R. Kaibyshev, 5 - Dynamic recrystallization in magnesium alloys, in: C. Bettles, M. Barnett (Eds.), Advances in Wrought Magnesium Alloys, Woodhead Publishing2012, pp. 186-225.

[78] A.G. Beer, M.R. Barnett, Microstructural Development during Hot Working of Mg-3Al-1Zn, Metallurgical and Materials Transactions A 38(8) (2007) 1856-1867.

[79] R. Kaibyshev, O. Sitdikov, Dynamic recrystallization of magnesium at ambient temperature, (1994).

[80] O. Muránsky, D.G. Carr, M.R. Barnett, E.C. Oliver, P. Šittner, Investigation of deformation mechanisms involved in the plasticity of AZ31 Mg alloy: In situ neutron diffraction and EPSC modelling, Materials Science and Engineering: A 496(1) (2008) 14-24.

[81] S. Yu, C. Liu, Y. Gao, S. Jiang, Z. Bao, Dynamic recrystallization mechanism of Mg-8.5Gd-2.5Y-0.4Zr alloy during hot ring rolling, Materials Characterization 131 (2017) 135-139.

[82] N. Stanford, M.D. Callaghan, B. de Jong, The effect of rare earth elements on the behaviour of magnesium-based alloys: Part 1—Hot deformation behaviour, Materials Science and Engineering: A 565 (2013) 459-468.

[83] O. Engler, An EBSD local texture study on the nucleation of recrystallization at shear bands in the alloy Al-3%Mg, Scripta Materialia 44(2) (2001) 229-236.

[84] W.Y. Yeung, J. Hirsch, M. Hatherly, Rolling and Annealing of Fine Grained 70:30 Brass, Textures and Microstructures 10 (1989) 923587.

88

[85] I. Ulacia, N.V. Dudamell, F. Gálvez, S. Yi, M.T. Pérez-Prado, I. Hurtado, Mechanical behavior and microstructural evolution of a Mg AZ31 sheet at dynamic strain rates, Acta Materialia 58(8) (2010) 2988-2998.

[86] M.A. Steiner, J.J. Bhattacharyya, S.R. Agnew, The origin and enhancement of {0001}〈112¯0〉

texture during heat treatment of rolled AZ31B magnesium alloys, Acta Materialia 95 (2015) 443-455.

[87] J.J. Bhattacharyya, S.R. Agnew, G. Muralidharan, Texture enhancement during grain growth of magnesium alloy AZ31B, Acta Materialia 86 (2015) 80-94.

[88] E.A. Ball, P.B. Prangnell, Tensile-compressive yield asymmetries in high strength wrought magnesium alloys, Scripta Metallurgica et Materialia 31(2) (1994) 111-116.

[89] K. Hantzsche, J. Bohlen, J. Wendt, K.U. Kainer, S.B. Yi, D. Letzig, Effect of rare earth additions on microstructure and texture development of magnesium alloy sheets, Scripta Materialia 63(7) (2010) 725-730.

[90] N. Stanford, Micro-alloying Mg with Y, Ce, Gd and La for texture modification—A comparative study, Materials Science and Engineering: A 527(10) (2010) 2669-2677.

[91] T. Al-Samman, X. Li, Sheet texture modification in magnesium-based alloys by selective rare earth alloying, Materials Science and Engineering: A 528(10) (2011) 3809-3822.

[92] N. Stanford, M.R. Barnett, The origin of “rare earth” texture development in extruded Mg-based alloys and its effect on tensile ductility, Materials Science and Engineering: A 496(1) (2008) 399-408.

[93] L.W.F. Mackenzie, M.O. Pekguleryuz, The recrystallization and texture of magnesium–zinc–cerium alloys, Scripta Materialia 59(6) (2008) 665-668.

[94] J.E. Burke, D. Turnbull, Recrystallization and grain growth, Progress in Metal Physics 3 (1952) 220-292.

[95] G.C. Hasson, C. Goux, Interfacial energies of tilt boundaries in aluminium. Experimental and theoretical determination, Scripta Metallurgica 5(10) (1971) 889-894.

[96] P.A. Beck, P.R. Sperry, Strain Induced Grain Boundary Migration in High Purity Aluminum, Journal

[96] P.A. Beck, P.R. Sperry, Strain Induced Grain Boundary Migration in High Purity Aluminum, Journal