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Self-equilibrated backstresses induce compensation between hardening and softening : Micromechanical and microstructural features

  • Qingge Xie*
  • , Jurij J. Sidor
  • , Junhe Lian
  • , Shuo Yin
  • , Yandong Wang
  • *Tämän työn vastaava kirjoittaja
  • University of Science and Technology Beijing
  • Eötvös Loránd University
  • Trinity College Dublin

Tutkimustuotos: Lehtiartikkeli › Article › Scientific › vertaisarvioitu

35 Sitaatiot (Scopus)

Abstrakti

For crystal plasticity formulation neglecting the strain gradients at the dislocation scale, backstresses are necessary to satisfy the mesoscopic stress equilibrium and strain compatibility requirements. Backstresses in a material point and those between neighboring points are treated separately. Physically backstresses can dynamically induce either hardening or softening effects to adjust the dislocation hardening of slip systems, whereas the sum of the stresses resulting in backstresses in the representative volume element (RVE) is zero. Backstress hardening suppresses certain slip activities, while backstress softening triggers excess dislocations. A two-phase brass is studied. Backstresses make the hard phase deform smaller and the soft phase deform more than those without employing backstresses in a model. In the former, more homogeneous lattice strain and higher yield stress are obtained. Backstress has limited effects on the evolution of the critical resolved shear stress and crystallographic texture. However, it is a major cause of the banded structures featuring sharp crystallographic contrasts which are not parallel to the slip planes. Tests indicate that backstress induces a serrated behavior at the early stages of deformation and induces the geometrically necessary bands (GNBs), which are parallel to the macroscopic axes.

AlkuperäiskieliEnglanti
Artikkeli143145
Sivumäärä17
JulkaisuMaterials Science and Engineering A: Structural Materials: Properties, Microstructures and Processing
Vuosikerta843
DOI - pysyväislinkit
TilaJulkaistu - 23 toukok. 2022
OKM-julkaisutyyppiA1 Alkuperäisartikkeli tieteellisessä aikakauslehdessä

Rahoitus

Project no. TKP2021-NVA-29 has been implemented with the support provided by the Ministry of Innovation and Technology of Hungary from the National Research, Development and Innovation Fund, financed under the TKP2021-NVA funding scheme (JJS). YDW thanks the Funds for Creative Research Groups of China (grant no. 51921001). QX thanks the funding from the National Natural Science Foundation of China (grant no. 51571025). Resources at the Spallation Neutron Source, U.S. DOE Office of Science User Facilities operated by ORNL, were used in this research. The authors thank the useful comments from Prof. Paul Van Houtte at KU Leuven in Belgium. Project no. TKP2021-NVA-29 has been implemented with the support provided by the Ministry of Innovation and Technology of Hungary from the National Research, Development and Innovation Fund , financed under the TKP2021-NVA funding scheme (JJS). YDW thanks the Funds for Creative Research Groups of China (grant no. 51921001 ). QX thanks the funding from the National Natural Science Foundation of China (grant no. 51571025 ). Resources at the Spallation Neutron Source, U.S. DOE Office of Science User Facilities operated by ORNL, were used in this research. The authors thank the useful comments from Prof. Paul Van Houtte at KU Leuven in Belgium.

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