Abstract:Magnetic Shape Memory Alloys (MSMAs) have been the subject of much research in recent years as potential high-actuation-energy multifunctional materials. In this work we analyze coupled magnetomechanical stability analysis of a variant reorientation mechanism for a single crystal based on a proposed 3-D magneto-mechanically coupled constitutive equations, derived in a consistent thermodynamic way. Discrete symmetry is considered to take into account single crystal anisotropy in the modeling. Analytical results… Show more
“…The constant stress component σ xx = σ , and Λ xx = ε max are known from the experiments. The model parameters A , B , C , D and Y (in (2.3)) are computed from the known material constants (see [31]). The evolution of the volume fraction ξ ( H y ) during forward reorientation is the solution of the following nonlinear algebraic equation: italicΦfalse(Hy,ξfalse)=π−Y=σεmax+μ0normalΔMHy−A2false(1+ξn1−false(1−ξfalse)n2false)+B−Y=0.…”
Section: The Magnetic Shape Memory Alloy Magneto-static Problemmentioning
Magnetic shape memory alloys (MSMAs) have drawn significant research attention as potential high actuation energy multi-functional materials. Such a dissipative material system can be considered as a solid continuum interacting with a magnetic field. A continuum-based phenomenological model provides a magneto-mechanical system of equations that simulates and predicts primary MSMA behaviours. In this work, we investigate the local symmetries of the MSMA system equations through the Lie group analysis. Symmetry breaking due to stable-unstable transition is analysed. The conservation laws are derived, and their physical meaning is scrutinized.
“…The constant stress component σ xx = σ , and Λ xx = ε max are known from the experiments. The model parameters A , B , C , D and Y (in (2.3)) are computed from the known material constants (see [31]). The evolution of the volume fraction ξ ( H y ) during forward reorientation is the solution of the following nonlinear algebraic equation: italicΦfalse(Hy,ξfalse)=π−Y=σεmax+μ0normalΔMHy−A2false(1+ξn1−false(1−ξfalse)n2false)+B−Y=0.…”
Section: The Magnetic Shape Memory Alloy Magneto-static Problemmentioning
Magnetic shape memory alloys (MSMAs) have drawn significant research attention as potential high actuation energy multi-functional materials. Such a dissipative material system can be considered as a solid continuum interacting with a magnetic field. A continuum-based phenomenological model provides a magneto-mechanical system of equations that simulates and predicts primary MSMA behaviours. In this work, we investigate the local symmetries of the MSMA system equations through the Lie group analysis. Symmetry breaking due to stable-unstable transition is analysed. The conservation laws are derived, and their physical meaning is scrutinized.
“…When analyzed as part of a complete magnetic circuit, properties of the MSM element affect the total reluctance and, hence the total magnetic field produced by coils and/or permanent magnets. Demagnetization effects related to MSM element's shape also make the understanding of magnetic field distribution in the MSM region based on measurement results challenging [10]. There is a considerable difference between the magnetic field in the MSM element and the magnetic field that can be measured in the air gap.…”
Section: B Msm Microstructure and Propertiesmentioning
confidence: 99%
“…There is a considerable difference between the magnetic field in the MSM element and the magnetic field that can be measured in the air gap. The significance of demagnetization and challenges associated with capturing related effects in analytical models have been mentioned numerously in publications e.g., [10]- [12]. However, effects related to geometry, non-homogeneity, anisotropy and non-linearity of magnetic characteristics can easily be taken into account in a FE model, a solution for which is obtained using numerical methods.…”
Section: B Msm Microstructure and Propertiesmentioning
confidence: 99%
“…9, it can be concluded that MSM reluctance always decreases with strain. However, the opposite is true for air gap reluctance (10). Therefore, the overall change in the reluctance of magnetic circuit depends on the ratio of these two reluctances.…”
This is the accepted version of the paper.This version of the publication may differ from the final published version. This article has been accepted for publication in a future issue of this journal, but has not been fully edited. Content may change prior to final publication. Magnetic shape memory (MSM) alloys are relatively new and very promising "smart" materials which respond to magnetic fields and exhibit the shape memory effect at room temperature. Maximum strain varies from 6 to 12% of the MSM element's length depending on its microstructure. The shape memory effect and magnetic field-induced reorientation of MSM twin variants in lowtemperature martensite phase are subject to an ongoing research for almost two decades. However, the magnetic field distribution in the MSM elements and effects of its varying magnetic permeability on bias magnetic field are not well studied. In this paper we present an extension to the existing modeling approach for MSM elements applicable to actuator design. The effects arising from single-crystal anisotropy and demagnetization effects due to non-homogeneous multi-variant MSM microstructure are studied and discussed. The proposed approach is validated by comparing computational results with previously reported measurement data.
Permanent repository linkIndex Terms-Magnetic shape memory (MSM) alloys, MSM actuators, electromagnetic analysis, non-homogeneous permeability, magnetic anisotropy
“…The induced anisotropy not only leads to different material properties in tension and compression but also to distinct and asymmetric stress–strain and transformation curves in tension and compression. Experimental reports have confirmed the realistic asymmetry phenomenon of the stress–strain behaviors of the SMAs [29–35], especially at high strain rates [36]. Based on the inelastic strains due to the martensitic transformation, variant reorientations, and martensite to austenite transformations under thermomechanical loads observed in tension/compression experiments of CuAlNi single crystals, Sittner and Novak [37] developed a simple constant stress averaging approach to model the SMA polycrystal deformation behaviors.…”
This paper is devoted to the investigation of the effects of the realistic tension–compression asymmetry and anisotropy of phase transformations of shape memory alloy wires embedded in composite sandwich plates with auxetic cores on the resulting nonlinear vibrations. A third-order zigzag description of the displacement field that takes into account the thickness variations of the flexible core and a novel three-dimensional dynamic elasticity stress and displacement correction is proposed and employed. The governing equations are extracted based on Hamilton’s principle and solved using an iterative finite element procedure. A comprehensive phase transformation algorithm and a constitutive model that are capable of accurately tracking the nested hysteresis loops and sub-loops and reverse loading of the shape memory alloy are proposed, considering the tension–compression anisotropy. Interactions of the core compliance, auxeticity, and especially, the transformations anisotropy on the dynamic responses are studied numerically and three-dimensional plots are presented for distributions of the martensite volume fraction. Results show that the realistic tension–compression anisotropy of the shape memory alloy material leads to results that are quite different from those based on the assumption of the symmetry of the material properties and significantly increases the differences between the damping roles of the shape memory alloy wires of the upper and lower layers of the sandwich plate.
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