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Journal articles on the topic 'Cyclic plasticity'

Author: Grafiati

Published: 4 June 2021

Last updated: 6 September 2023

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1

Moosbrugger, J. C., and N. Ohno. "Multiaxial plasticity, cyclic plasticity and viscoplasticity." International Journal of Plasticity 16, no. 3-4 (January 2000): 223–24. http://dx.doi.org/10.1016/s0749-6419(99)00062-5.

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2

Šumarac, Dragoslav, and Zoran Perović. "Cyclic plasticity of trusses." Archive of Applied Mechanics 85, no. 9-10 (December 3, 2014): 1513–26. http://dx.doi.org/10.1007/s00419-014-0954-7.

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3

Tóth, L. S., A. Molinari, and N. Zouhal. "Cyclic plasticity phenomena as predicted by polycrystal plasticity." Mechanics of Materials 32, no. 2 (February 2000): 99–113. http://dx.doi.org/10.1016/s0167-6636(99)00040-x.

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4

Chaboche, J. L. "Constitutive equations for cyclic plasticity and cyclic viscoplasticity." International Journal of Plasticity 5, no. 3 (January 1989): 247–302. http://dx.doi.org/10.1016/0749-6419(89)90015-6.

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5

Lou, J., P. Shrotriya, and W. O. Soboyejo. "A Cyclic Microbend Study on LIGA Ni Microelectromechanical Systems Thin Films." Journal of Engineering Materials and Technology 127, no. 1 (January 1, 2005): 16–22. http://dx.doi.org/10.1115/1.1836767.

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This paper presents the results of recent studies of cyclic microbend experiments and their consequences for plasticity length-scale phenomena in LIGA Ni microelectromechanical systems (MEMS) thin films. The strain–life fatigue behavior of LIGA Ni thin films is studied by performing fully reversed cyclic microbend experiments that provide insights into cyclic stress/strain evolution and cyclic failure phenomena. The effects of cyclic deformation on the plasticity length-scale parameters are also considered within the context of strain gradient plasticity theories. The implications of the results are then discussed for the analysis of plasticity and cyclic deformation in MEMS structures and other microscale systems.

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6

Brocks, Wolfgang, and Dirk Steglich. "Damage Models for Cyclic Plasticity." Key Engineering Materials 251-252 (October 2003): 389–98. http://dx.doi.org/10.4028/www.scientific.net/kem.251-252.389.

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7

Mikhalevich, V. M. "Plasticity with cyclic hot working." Strength of Materials 26, no. 6 (June 1994): 407–12. http://dx.doi.org/10.1007/bf02209409.

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8

HASHIGUCHI, Koichi. "Assessment of cyclic plasticity models." Proceedings of The Computational Mechanics Conference 2022.35 (2022): GS—01. http://dx.doi.org/10.1299/jsmecmd.2022.35.gs-01.

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9

Chiang, Dar-Yun. "A Phenomenological Model for Cyclic Plasticity." Journal of Engineering Materials and Technology 119, no. 1 (January 1, 1997): 7–11. http://dx.doi.org/10.1115/1.2805979.

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A phenomenological model is proposed for cyclic plasticity based on the concept of distributed elements, which is capable of reflecting microstructural behavior of real materials under multiaxial cyclic loading conditions. By investigating the detailed behavior of the model, various important phenomena and effects of materials in cyclic plasticity can be elucidated. Generalization of the model is also done to include cyclic hardening effects. A thorough understanding of these complicated response mechanisms and material properties provides useful insight and guidelines for validating analytical models and for performing experimental studies in the related areas of cyclic plasticity.

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10

Sajjad, Hafiz Muhammad, Stefanie Hanke, Sedat Güler, Hamad ul Hassan, Alfons Fischer, and Alexander Hartmaier. "Modelling Cyclic Behaviour of Martensitic Steel with J2 Plasticity and Crystal Plasticity." Materials 12, no. 11 (May 31, 2019): 1767. http://dx.doi.org/10.3390/ma12111767.

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In order to capture the stress-strain response of metallic materials under cyclic loading, it is necessary to consider the cyclic hardening behaviour in the constitutive model. Among different cyclic hardening approaches available in the literature, the Chaboche model proves to be very efficient and convenient to model the kinematic hardening and ratcheting behaviour of materials observed during cyclic loading. The purpose of this study is to determine the material parameters of the Chaboche kinematic hardening material model by using isotropic J2 plasticity and micromechanical crystal plasticity (CP) models as constitutive rules in finite element modelling. As model material, we chose a martensitic steel with a very fine microstructure. Thus, it is possible to compare the quality of description between the simpler J2 plasticity and more complex micromechanical material models. The quality of the results is rated based on the quantitative comparison between experimental and numerical stress-strain hysteresis curves for a rather wide range of loading amplitudes. It is seen that the ratcheting effect is captured well by both approaches. Furthermore, the results show that concerning macroscopic properties, J2 plasticity and CP are equally suited to describe cyclic plasticity. However, J2 plasticity is computationally less expensive whereas CP finite element analysis provides insight into local stresses and plastic strains on the microstructural length scale. With this study, we show that a consistent material description on the microstructural and the macroscopic scale is possible, which will enable future scale-bridging applications, by combining both constitutive rules within one single finite element model.

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11

Zhang, Rui, and Sun Yi. "Cyclic Plasticity and Fatigue Crack Growth." Key Engineering Materials 324-325 (November 2006): 603–6. http://dx.doi.org/10.4028/www.scientific.net/kem.324-325.603.

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The relation between material’s cyclic plastic behavior and fatigue crack growth is investigated. The present model is proposed on the dislocation-free zone (DFZ) theory. A cohesive zone theory is developed to determine the stress field of the DFZ and the value of J-integer under cyclic loading. The crack growth criterion is proposed based on J-integral. The calculated curve of fatigue crack growth rate da/dN is agreement with the general propagation pattern and the predicted threshold accords with the experiment threshold well. It is found that the near threshold characteristics are most determined by the cyclic deformation behavior of the material. The relation between fatigue crack growth threshold and material’s cyclic hardening behavior is discussed.

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12

Su, Luo Chuan, Jian Guo Li, Wei Xu Zhang, and Tie Jun Wang. "Effect of Temperature-Dependent Properties on Cyclic Plasticity of Bond Coat in Thermal Barrier Systems." Key Engineering Materials 535-536 (January 2013): 193–96. http://dx.doi.org/10.4028/www.scientific.net/kem.535-536.193.

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The accumulation of cyclic plasticity in bond coat (BC) is a key factor controlling the displacement instability of the thermally grown oxide (TGO) in thermal barrier systems. The cyclic plasticity is affected by the component material properties, which vary observably with the service temperature. A numerical model with the behavior of creep and thermal growth in TGO under thermal cycling is used to explore the effect of temperature-dependent properties on cyclic plasticity in BC. The influence of temperature-dependent Young's modulus of thermal barrier coating (TBC), TGO, BC and substrate, thermal expansion coefficient of TBC, BC and substrate, and the yield strength of BC on cyclic plasticity in BC is discussed respectively.

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13

Du, Xin, Xiaochong Lu, Siyao Shuang, Zhangwei Wang, Qi-lin Xiong, Guozheng Kang, and Xu Zhang. "Cyclic Plasticity of CoCrFeMnNi High-Entropy Alloy (HEA): A Molecular Dynamics Simulation." International Journal of Applied Mechanics 13, no. 01 (January 2021): 2150006. http://dx.doi.org/10.1142/s175882512150006x.

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The CoCrFeMnNi high-entropy alloy (HEA) is a potential structural material, whose cyclic plasticity is essential for its safety assessment in service. Here, the effects of twin boundaries (TBs) and temperature on the cyclic plasticity of CoCrFeMnNi HEA were studied by the molecular dynamics (MD) simulation. The simulation results showed that a significant amount of lattice disorders were generated due to the interactions between partial dislocations in CoCrFeMnNi HEA during the cyclic deformation. Lattice disorder impeded the reverse movement of dislocations and then weakened Bauschinger’s effect in the HEA. The cyclic plasticity of CoCrFeMnNi HEA, especially Bauschinger’s effect, depends highly on the temperature and pre-existing TBs. Such dependence lies in the effects of temperature and pre-existing TBs on the extent of lattice disorder. This study helps further understand the cyclic plasticity of CoCrFeMnNi HEA from the atomic scale.

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14

Kobayashi, Takumi, Kohshiroh Kitayama, Takeshi Uemori, and Fusahito Yoshida. "Description of Planer Anisotropy and Cyclic Plasticity Behavior of Aluminum Sheet Based on Crystal Plasticity Theory." Applied Mechanics and Materials 117-119 (October 2011): 1397–401. http://dx.doi.org/10.4028/www.scientific.net/amm.117-119.1397.

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In sheet metal forming, the anisotropy and the Bauschinger effect of sheets affect greatly their formability. This paper discusses how the planar anisotropy and cyclic plastic behavior (the Bauschnger effect and cyclic workhardening characteristics) correlate with the crystallographic texture based on the crystal plasticity analysis on A5052-O sheet. The analytical predictions of r-values and the cyclic stress-strain responses are compared with the experimental observations (S. Tamura et al., Materials Trans, 52-5 (2011), pp.868-875).

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15

MINAGAWA, Masaru, Takeo NISHIWAKI, and Nobutoshi MASUDA. "Modelling cyclic plasticity of structural steels." Doboku Gakkai Ronbunshu, no. 386 (1987): 145–54. http://dx.doi.org/10.2208/jscej.1987.386_145.

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16

Bondar, V. S., D. R. Abashev, and D. U. Fomin. "THEORIES OF PLASTICITY UNDER CYCLIC LOADINGS." Problems of Strength and Plasticity 80, no. 1 (2018): 31–40. http://dx.doi.org/10.32326/1814-9146-2018-80-1-31-40.

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17

Tsakmakis, Aris, and Michael Vormwald. "Configurational forces in cyclic metal plasticity." MATEC Web of Conferences 300 (2019): 08009. http://dx.doi.org/10.1051/matecconf/201930008009.

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The configurational force concept is known to describe adequately the crack driving force in linear fracture mechanics. It seems to represent the crack driving force also for the case of elastic-plastic material properties. The latter has been recognized on the basis of thermodynamical considerations. In metal plasticity, real materials exhibit hardening eﬀects when suﬃciently large loads are applied. Von Mises yield function with isotropic and kinematic hardening is a common assumption in many models. Kinematic and isotropic hardening turn out to be very important whenever cyclic loading histories are applied. This holds equally regardless of whether the induced deformations are homogeneous or non-homogeneous. The aim of the present paper is to discuss the eﬀect of nonlinear isotropic and kinematic hardening on the response of the configurational forces and related parameters in elastic-plastic fracture problems.

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18

Borja, Ronaldo I., and Alexander P. Amies. "Multiaxial Cyclic Plasticity Model for Clays." Journal of Geotechnical Engineering 120, no. 6 (June 1994): 1051–70. http://dx.doi.org/10.1061/(asce)0733-9410(1994)120:6(1051).

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19

McDowell, David L. "Simple Experimentally Motivated Cyclic Plasticity Model." Journal of Engineering Mechanics 113, no. 3 (March 1987): 378–97. http://dx.doi.org/10.1061/(asce)0733-9399(1987)113:3(378).

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20

POMMIER, S. "Cyclic plasticity and variable amplitude fatigue." International Journal of Fatigue 25, no. 9-11 (September 2003): 983–97. http://dx.doi.org/10.1016/s0142-1123(03)00137-3.

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21

Lukáš, P., and L. Kunz. "Cyclic plasticity and substructure of metals." Materials Science and Engineering: A 322, no. 1-2 (January 2002): 217–27. http://dx.doi.org/10.1016/s0921-5093(01)01132-7.

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22

Yoshida, Fusahito. "A constitutive model of cyclic plasticity." International Journal of Plasticity 16, no. 3-4 (January 2000): 359–80. http://dx.doi.org/10.1016/s0749-6419(99)00058-3.

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23

Niordson, Christian F., and Brian Nyvang Legarth. "Strain gradient effects on cyclic plasticity." Journal of the Mechanics and Physics of Solids 58, no. 4 (April 2010): 542–57. http://dx.doi.org/10.1016/j.jmps.2010.01.007.

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24

MUGHRABI, H. "Cyclic plasticity and fatigue of metals." Le Journal de Physique IV 03, no. C7 (November 1993): C7–659—C7–668. http://dx.doi.org/10.1051/jp4:19937105.

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25

Xianghe, Peng, Gao Zhihui, and Fan Jinghong. "Constitutive modelling of nonproportional cyclic plasticity." Acta Mechanica Sinica 8, no. 3 (August 1992): 244–52. http://dx.doi.org/10.1007/bf02489248.

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26

Das, Arpan. "Slip System Activity During Cyclic Plasticity." Metallurgical and Materials Transactions A 45, no. 7 (April 15, 2014): 2927–30. http://dx.doi.org/10.1007/s11661-014-2295-0.

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27

Halama, Radim, Jaromír Fumfera, Petr Gál, Tadbhagya Kumar, and Alexandros Markopoulos. "Modelling the Strain Range Dependent Cyclic Hardening of SS304 and 08Ch18N10T Stainless Steel with a Memory Surface." Metals 9, no. 8 (July 26, 2019): 832. http://dx.doi.org/10.3390/met9080832.

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This paper deals with the development of a cyclic plasticity model suitable for predicting the strain range dependent behavior of austenitic steels. The proposed cyclic plasticity model uses the virtual back-stress variable corresponding to a cyclically stable material under strain control. This new internal variable is defined by means of a memory surface introduced in the stress space. The linear isotropic hardening rule is also superposed. First, the proposed model was validated on experimental data published for the SS304 material (Kang et al. Constitutive modeling of strain range dependent cyclic hardening. Int J Plast 19 (2003) 1801–1819). Subsequently, the proposed cyclic plasticity model was applied to own experimental data from uniaxial tests realized on 08Ch18N10T at room temperature. The new cyclic plasticity model can be calibrated by the relatively simple fitting procedure that is described in the paper. A comparison between the results of a numerical simulation and the results of real experiments demonstrates the robustness of the proposed approach.

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28

Wang, Haiyang, and M. E. Barkey. "Strain Space Formulation of the Armstrong-Frederick Family of Plasticity Models." Journal of Engineering Materials and Technology 120, no. 3 (July 1, 1998): 230–35. http://dx.doi.org/10.1115/1.2812348.

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Strain space based plasticity models have certain advantages in theoretical development and numerical implementation. Previous efforts have been made to formulate cyclic plasticity models in strain space using the idea of multiple-yield surface theory. Recently, however, Armstrong-Frederick type plasticity models have received increasingly more attention because of their enhanced performance in predicting ratchetting behavior. In this paper, the strain space formulation of the Armstrong-Frederick family of cyclic plasticity models is established, and several representative strain controlled loading paths are used to compare the results from the proposed formulation and previous experimental data. The excellent agreement suggests the proposed strain space formulation is very promising in strain controlled cyclic plasticity such as finite element analysis, strain gage rosette applications, and multiaxial notch analysis using pseudo-stress or pseudo-strain approaches.

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29

Polák, Jaroslav, Martin Petrenec, Jiří Man, and Tomáš Kruml. "Cyclic Plasticity and Cyclic Creep in Austenitic-Ferritic Duplex Steel." Key Engineering Materials 465 (January 2011): 431–34. http://dx.doi.org/10.4028/www.scientific.net/kem.465.431.

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Smooth specimens made from austenitic-ferritic duplex steel were subjected to constant stress amplitude loading with positive mean stresses. Hysteresis loops were recorded during the fatigue life and plastic strain amplitude and cyclic creep rate were determined. Fatigue hardening/softening curves, cyclic creep curves and cyclic stress-strain curves for different positive mean stresses were evaluated. Typical dislocation structures developed in both phases of the duplex steel were identified using TEM, compared with the saturated plastic strain amplitude and correlated with the decrease of the cyclic creep rate during cycling and the slope of the cyclic stress-strain curve.

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30

Mayama, Tsuyoshi, Katsuhiko Sasaki, and Yoshihiro Narita. "Quantitative Evaluation of Dislocation Structure Induced by Cyclic Plasticity." Key Engineering Materials 345-346 (August 2007): 49–52. http://dx.doi.org/10.4028/www.scientific.net/kem.345-346.49.

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In the present study, a new approach is conducted to evaluate dislocation structure induced by cyclic plasticity. First, cyclic plastic loading tests are carried out up to 100 cycles with three different small strain amplitudes on SUS316L stainless steel at room temperature. The test result presents the dependence of the strain amplitude on cyclic hardening and softening behaviors. Specifically, it is found that the cyclic loading test with strain amplitude of 0.25% shows both cyclic hardening and cyclic softening, while the cyclic loading tests with strain amplitudes of 0.75% and 1.0% show no cyclic softening. Secondly, the dislocation structures of the specimens after cyclic loading are observed by using a transmission electron microscope (TEM), and this observation reveals that the dislocation structure after cyclic loading test depends on the strain amplitude. Finally, a quantitative evaluation method of the dislocation structure is also proposed. The TEM images are converted into binary images and the resolution dependence of the generated binary image is used to visualize the characteristics of the dislocation structure. The relationship between strain amplitudes of cyclic plasticity and dislocation structure organization is clarified by the evaluation method. Finally, the heterogeneity of the dislocation structure is discussed.

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31

Devaney, Ronan J., Heiner Oesterlin, Padraic E. O’Donoghue, and Sean B. Leen. "Cyclic plasticity and low cycle fatigue damage characterisation of thermally simulated X100Q heat affected zone." MATEC Web of Conferences 165 (2018): 03002. http://dx.doi.org/10.1051/matecconf/201816503002.

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This paper presents the cyclic plasticity and low cycle fatigue (LCF) damage characterisation of thermally simulated heat affected zone (HAZ) for API 5L X100Q weldments. Microstructures representative of the HAZ for two cooling rates are generated using a Gleeble thermomechanical simulator for manufacture of strain-controlled cyclic plasticity test specimens. The simulated HAZ specimens are subjected to a strain controlled test programme which examines the cyclic effects of strain-range and the tensile response at room temperature. A modified version of the Chaboche rate independent plasticity model, which accounts for early stage damage is implemented to characterise the cyclic plasticity response, including isotropic and kinematic hardening effects. The constitutive parameters are fitted to experimental data using an optimisation procedure developed within a MATLAB code. The measured response of the simulated HAZ specimens is compared to that of the X100Q parent material (PM), and the simulated HAZ is shown to share the early stage fatigue damage behaviour of the PM, but exhibits significantly a higher yield and cyclic strength.

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32

Mo, Yafei, Rou Du, and Xiaoming Liu. "Effect of mixed plastic hardening on the cyclic contact between a sphere and a rigid flat." Journal of Physics: Conference Series 2285, no. 1 (June 1, 2022): 012018. http://dx.doi.org/10.1088/1742-6596/2285/1/012018.

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Abstract This paper studies the effect of mixed plasticity mode (combined with isotropic and kinematic hardening law) on the cyclic contact between an elastic-plastic sphere and a rigid flat. Assuming power-law hardening with different levels of mixed plasticity for the sphere, we derived a semi-analytical expression of load versus interference during the first loading and unloading process. During cyclic loading, our results indicate that the isotropic plasticity model shows no variation of residual interference, while kinematic plasticity has the cyclic effect on the residual interference, and this effect is bigger for the material with a higher hardening exponent. In addition, we provided the semi-analytical expression for the evolution of residual interference, which is accurate for the strain hardening exponent from 0.1 to 0.5.

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33

HAMADA, Kazuaki, Kenji YOSHIYAMA, Takeshi UEMORI, and Fusahito YOSHIDA. "Numerical Simulation of Cyclic Plasticity by Finite Element Crystal Plasticity Model." Proceedings of Conference of Chugoku-Shikoku Branch 2004.42 (2004): 119–20. http://dx.doi.org/10.1299/jsmecs.2004.42.119.

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34

Ohno, N., and Y. Kachi. "A Constitutive Model of Cyclic Plasticity for Nonlinear Hardening Materials." Journal of Applied Mechanics 53, no. 2 (June 1, 1986): 395–403. http://dx.doi.org/10.1115/1.3171771.

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A constitutive model is proposed for cyclic plasticity of nonlinear hardening materials. The concept of a cyclic nonhardening range, which enables us to describe the dependence of cyclic hardening on the amplitude of cyclic straining or stressing, is employed together with the idea of a two-surface plasticity model. Results of the proposed model are compared with experiments of 304 and 316 stainless steels in several cases of cyclic loading in which mean strain is zero or nonzero and strain limits are fixed or variable. Thus, it is shown that the model successfully describes both the cyclic hardening phenomenon and the transient elastoplastic behavior after initial and reverse yields of these materials. The capability of the model to provide nonlinear cyclic stress-strain curves is also discussed.

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35

Mayama, Tsuyoshi, Katsuhiko Sasaki, and Hiromasa Ishikawa. "GSW0044 Interaction between cyclic plasticity and creep of type 304 stainless steel." Abstracts of ATEM : International Conference on Advanced Technology in Experimental Mechanics : Asian Conference on Experimental Mechanics 2003.2 (2003): _GSW0044–1—_GSW0044–6. http://dx.doi.org/10.1299/jsmeatem.2003.2._gsw0044-1.

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36

Dahl, Karina R., Jason T. DeJong, Ross W. Boulanger, Robert Pyke, and Douglas Wahl. "Characterization of an alluvial silt and clay deposit for monotonic, cyclic, and post-cyclic behavior." Canadian Geotechnical Journal 51, no. 4 (April 2014): 432–40. http://dx.doi.org/10.1139/cgj-2013-0057.

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This paper presents a detailed characterization of the monotonic, cyclic, and post-cyclic behavior of two strata within a recent Holocene alluvial deposit of silty sand, sandy silt, silt, and clay. Stratum A is composed predominantly of very soft clay and very loose silt with plasticity indices ranging from 5 to 27, whereas stratum B is composed predominantly of very loose silty sand and sandy silt with plasticity indices ranging from 0 to 10. Characterization included in situ testing, undisturbed soil sampling and laboratory testing, and a field surcharge test section. Consolidation tests and monotonic, cyclic, and post-cyclic direct simple shear tests were used to evaluate the effects of varying the consolidation stress, consolidation stress history, and initial static shear stress ratio. The field and laboratory test data show distinct differences in behavior between the two soil strata, which can be related to their different index test characteristics. These results are compared with their respective behaviors predicted using common engineering correlations. The field and laboratory test data summarized herein contribute to the database and understanding of the monotonic, cyclic, and post-cyclic behaviors of low-plasticity fine-grained soils.

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37

Tu, Wen Feng, Xiao Gui Wang, and Zeng Liang Gao. "Modeling of Fatigue Crack Growth Based on Two Cyclic Plasticity Models." Advanced Materials Research 44-46 (June 2008): 111–18. http://dx.doi.org/10.4028/www.scientific.net/amr.44-46.111.

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Based on two different cyclic plasticity models, fatigue crack growth for 16MnR steel specimens is simulated by using the same multi-axial fatigue damage criterion. The first plasticity model is the Jiang and Sehitoglu model and the second plasticity model is the simple nonlinear kinematic hardening model. The elastic-plastic stress-strain field near the crack tip is obtained respectively by using the two plasticity models. According to the same fatigue criterion, different fatigue damage near the crack tip is determined on the basis of stress-strain responses. The first plasticity model can accurately capture cyclic plasticity deformation behavior and predictions of fatigue crack growth rate are in agreement with the experimental results. However, lots of material constants in the model need to be fitted and more experimental tests should be conducted. The second plasticity model is very simple. The parameters of the model can be acquired easily by uniaxial fatigue tests. Compared with experimental data, the prediction results of fatigue crack growth rate lead to some errors by adopting the second plasticity model.

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38

Babaei, A., MM Mashhadi, and F. Mehri Sofiani. "Crystal plasticity modeling of grain refinement in aluminum tubes during tube cyclic expansion-extrusion." Proceedings of the Institution of Mechanical Engineers, Part L: Journal of Materials: Design and Applications 232, no. 6 (March 4, 2016): 481–94. http://dx.doi.org/10.1177/1464420716634745.

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In the present study, a crystal plasticity finite element model was developed for simulating the microstructure evolution and grain refinement during tube cyclic expansion-extrusion as a severe plastic deformation method for tubular materials. A new approach was proposed for extracting the real deformation history of a representative volume element during severe plastic deformation methods. The deformation history of a representative volume element during four cycles of tube cyclic expansion-extrusion was extracted by the proposed approach. Then, in a crystal plasticity finite element model, the deformation history was applied to a two-dimensional polycrystalline representative volume element with randomly assigned crystalline orientations. The intergranular interactions between grains and the intragranular orientation gradients were successfully simulated by the crystal plasticity finite element model. The distribution of misorientation angles, the evolution of grain boundaries, and the achieved average grain size after different cycles of tube cyclic expansion-extrusion were investigated by the crystal plasticity finite element model. On the other hand, ultrafine grained aluminum tubes were processed by four cycles of tube cyclic expansion-extrusion and the grain size of the processed tubes was studied by scanning electron microscopy observations and X-ray diffraction analyses. The experimental and predicted (by crystal plasticity finite element model) average grain sizes were compared.

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39

Yip, Tick Hon, and Zhi Rui Wang. "Cyclic Plasticity of Precipitation-Hardenable Stainless Steel." Key Engineering Materials 233-236 (January 2003): 275–80. http://dx.doi.org/10.4028/www.scientific.net/kem.233-236.275.

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40

Iai, Susumu, Yasuo Matsunaga, and Tomohiro Kameoka. "Strain Space Plasticity Model for Cyclic Mobility." Soils and Foundations 32, no. 2 (June 1992): 1–15. http://dx.doi.org/10.3208/sandf1972.32.2_1.

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41

OBATAYA, Yoichi. "Effect of thermal fluctuations in cyclic plasticity." Transactions of the Japan Society of Mechanical Engineers Series A 52, no. 480 (1986): 2087–94. http://dx.doi.org/10.1299/kikaia.52.2087.

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42

Rui, Y., and C. T. Sun. "Cyclic Plasticity in AS4/PEEK Composite Laminates." Journal of Thermoplastic Composite Materials 6, no. 4 (October 1993): 312–22. http://dx.doi.org/10.1177/089270579300600404.

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43

HASHIGUCHI, Koichi. "2319 Comparison of Various Cyclic Plasticity Models." Proceedings of The Computational Mechanics Conference 2011.24 (2011): 672–74. http://dx.doi.org/10.1299/jsmecmd.2011.24.672.

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44

Vucetic, Mladen, and Ricardo Dobry. "Effect of Soil Plasticity on Cyclic Response." Journal of Geotechnical Engineering 117, no. 1 (January 1991): 89–107. http://dx.doi.org/10.1061/(asce)0733-9410(1991)117:1(89).

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45

Zhang, Z. "Anisothermal cyclic plasticity modelling of martensitic steels." International Journal of Fatigue 24, no. 6 (June 2002): 635–48. http://dx.doi.org/10.1016/s0142-1123(01)00182-7.

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46

Abdul-Latif, A. "Constitutive equations for cyclic plasticity of Waspaloy." International Journal of Plasticity 12, no. 8 (January 1996): 967–85. http://dx.doi.org/10.1016/s0749-6419(96)00037-x.

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47

Chaboche, J. L. "Time-independent constitutive theories for cyclic plasticity." International Journal of Plasticity 2, no. 2 (January 1986): 149–88. http://dx.doi.org/10.1016/0749-6419(86)90010-0.

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Jiang, Yanyao, and Jixi Zhang. "Benchmark experiments and characteristic cyclic plasticity deformation." International Journal of Plasticity 24, no. 9 (September 2008): 1481–515. http://dx.doi.org/10.1016/j.ijplas.2007.10.003.

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Castelluccio, Gustavo M., and David L. McDowell. "Mesoscale cyclic crystal plasticity with dislocation substructures." International Journal of Plasticity 98 (November 2017): 1–26. http://dx.doi.org/10.1016/j.ijplas.2017.06.002.

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Xu, Biqiang, and Yanyao Jiang. "A cyclic plasticity model for single crystals." International Journal of Plasticity 20, no. 12 (December 2004): 2161–78. http://dx.doi.org/10.1016/j.ijplas.2004.05.003.

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