Full Length ArticleFundamental analysis of deformation behavior in core-shell heterostructured materials
Graphical abstract
Introduction
Heterostructures have been extensively researched to improve conventional design strategies and achieve more advanced mechanical properties by controlling the microstructures using appropriate processing techniques [1], [2], [3], [4], [5]. The design of microstructural heterogeneity should consider several microstructural features to enhance strength, ductility, and fracture toughness. Although deformation behavior is mainly associated with factors that influence the microstructure–mechanical property relationship of heterostructures, the fundamental deformation behavior of these materials has not been quantitatively elucidated thus far.
Microstructural heterogeneities, such as grain size, phase, and morphology, lead to the formation of a strain gradient during plastic deformation owing to interfacial strain incompatibility between the soft and hard domains. Consequently, hetero-deformation induces a strain partition that preferentially deforms the soft domain by forming geometrically necessary dislocations (GNDs). Thus, the plastic incompatibility between the soft and hard domains is observable as a gradient distribution of GNDs in the soft domain at the interface [6]. As deformation proceeds, the accumulated GNDs promote hetero-deformation induced (HDI) hardening. This indicates that a heterogeneous interface diretly results in strain incompatibility and GND accumulations, and promotes HDI hardening [7], [8]. In a recent study, the phase boundaries in the designed dual-phase alloys were investigated with respect to their influence on mechanical properties due to strain accommodation that is dependent on phase morphology and size as an expansion of the grain level [9]. The phase morphology rather than phase orientation induces different microscopic deformation behaviors with respect to the width of the phase boundary affected zone where GNDs are piled-up; a narrow width of the soft phase enclosed by the hard phase can have a higher density of phase boundary affected zone in the entire soft phase region.
Furthermore, the importance of the phase arrangement was studied from the core–shell structure designed assuming the same phase interfacial region in this study. A structure composed of a soft matrix and hard particle is defined as a hard-core (HC), soft-shell structure [10], [11], [12], [13]. Conversely, a structure composed of a hard matrix and soft particle is defined as a soft-core (SC), hard-shell structure, which was proposed by Ameyama et al. based on the characteristic morphology and mechanical properties of these materials [14], [15]. The two types of core–shell structures are evaluated by applying a dislocation-based constitutive model using the finite element method (FEM) to verify the importance of the relationship between microstructural engineering and mechanical properties in the design of optimal heterostructures. In particular, because this proposed dislocation-based constitutive model can consider the evolution of GNDs, unlike the simple constitutive model that does not consider the physical meaning and spatial distribution of GNDs, the effect of additional HDI hardening by strain incompatibility was successfully estimated at the domain boundary.
Section snippets
Finite element method modeling using the physical-based deformation mechanism
The flow stress related to dislocation interactions is calculated by summing the frictional stress, dislocation forest hardening, and HDI hardening as follows [16], [17]:
where , and are the frictional stress, geometrical arrangement of the dislocation, Taylor factor, shear modulus, magnitude of the Burgers vector, statistically stored dislocation (SSD) density, and HDI stress, respectively.
During plastic deformation, the flow stress is expressed by the
Results and discussion
The uniaxial tensile mode was applied to determine the mechanical properties of the SC and HC structures using two types of constitutive models. The first constitutive model considers only the SSD behavior, whereas the second model additionally considers the GND behavior along with the SSDs as explained above. The obtained true stress–strain curves of the HC and SC structures are shown as solid lines (only SSDs) and dotted lines (SSDs and GNDs together) in Fig. 3. Moreover, Fig. 4 shows the
Conclusion
Common core–shell heterostructures, including the SC and HC structures composed of the same volume fraction of the soft and hard domains, were analyzed to expand fundamental understandings of microstructure design based on the dislocation-based deformation mechanism using the developed FEM model. The SC structure had significantly better mechanical properties than the HC structure owing to the uniform deformation. Conversely, the GND-evolved HC structure had improved mechanical properties owing
CRediT authorship contribution statement
Yongju Kim: Conceptualization, Software, Visualization, Writing – original draft. Gang Hee Gu: Investigation. Hyoung Seop Kim: Conceptualization, Supervision, Funding acquisition, Writing – review & editing.
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
This study was supported by the National Research Foundation (NRF) of Korea under Grants [NRF- 2021R1A2C3006662] and [NRF-2022R1A5A1030054] funded by the Ministry of Science, ICT and Future Planning (MSIP) of the Korean government.
References (27)
- et al.
A new strategy for fabrication of unique heterostructured titanium laminates and visually tracking their synchronous evolution of strain partitions versus microstructure
J. Mater. Sci. Technol.
(2022) - et al.
Fabrication of multi-gradient heterostructured CoCrFeMnNi high-entropy alloy using laser metal deposition
Mater. Sci. Eng. A.
(2022) - et al.
Aged metastable high-entropy alloys with heterogeneous lamella structure for superior strength-ductility synergy
Acta Mater.
(2020) - et al.
High-entropy alloys with heterogeneous microstructure: processing and mechanical properties
Prog. Mater. Sci.
(2022) - et al.
In-situ investigation of the deformation behavior of heterogeneous-cell-structured Ni with a good strength-ductility balance
Mater. Sci. Eng. A.
(2022) - et al.
Extra strengthening in a coarse/ultrafine grained laminate: Role of gradient interfaces
Int. J. Plast.
(2019) - et al.
Effect of phase morphology on microscopic deformation behavior of Mg–Li–Gd dual-phase alloys
Mater. Sci. Eng. A.
(2021) - et al.
Particle distribution in cast metal matrix composites - Part I
J. Mater. Process. Technol.
(2002) - et al.
Effects of matrix microstructure and particle distribution on fracture of an aluminum metal matrix composite
Mater. Sci. Eng. A.
(1989) - et al.
Heterogeneous evolution of lattice defects leading to high strength and high ductility in harmonic structure materials through atomic and dislocation simulations
Acta Mater.
(2022)
Deformation behavior of lightweight clad sheet: experiment and modeling
Mater. Sci. Eng. A.
Physics and phenomenology of strain hardening: the FCC case
Prog. Mater. Sci.
A unified phenomenological description of work hardening and creep based on one-parameter models
Acta Metall.
Cited by (3)
Fabrication of spatially-variable heterostructured CoCrFeMnNi high entropy alloy by laser processing
2024, Materials Science and Engineering: AShear Deformation Behavior of Heterostructured Materials: Experimental and Numerical Analyses
2023, Metals and Materials International