2020
DOI: 10.1007/s00419-020-01778-0
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Transversely isotropic magnetoactive elastomers: theory and experiments

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Cited by 7 publications
(8 citation statements)
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“…Considering the Equations (2)–(4) in Equation (1), with the assumption of the Neo-Hookean hyperelastic material model for a nearly incompressible magnetoelastic medium [ 48 , 49 ] and linear elastic wave motion [ 50 , 51 ], and also considering field-dependent material properties of magnetorheological elastomers [ 49 ], the governing equation of motion for a unit cell in the presence of induced magnetic flux density, , can be evaluated as: where the and are the field-dependent mass and stiffness matrices of the unit cell, respectively, which are dependent on external magnetic flux ( ), elastic modulus ( ), unit cell geometry, density, and magnetic susceptibility ( ) of the filled elastomer with a specific amount of iron volume fraction.…”
Section: Methodsmentioning
confidence: 99%
“…Considering the Equations (2)–(4) in Equation (1), with the assumption of the Neo-Hookean hyperelastic material model for a nearly incompressible magnetoelastic medium [ 48 , 49 ] and linear elastic wave motion [ 50 , 51 ], and also considering field-dependent material properties of magnetorheological elastomers [ 49 ], the governing equation of motion for a unit cell in the presence of induced magnetic flux density, , can be evaluated as: where the and are the field-dependent mass and stiffness matrices of the unit cell, respectively, which are dependent on external magnetic flux ( ), elastic modulus ( ), unit cell geometry, density, and magnetic susceptibility ( ) of the filled elastomer with a specific amount of iron volume fraction.…”
Section: Methodsmentioning
confidence: 99%
“…In this regard, classical invariants have been used in some studies to model the behavior of transversely isotropic materials. [149,[151][152][153] For hyperelastic transversely isotropic materials, Bustamante [149] used the isothermal Helmholtz free energy density function, Ω, which depends on ten invariants as follows…”
Section: Continuum-based Modelsmentioning
confidence: 99%
“…The first three invariants (I 1 -I 3 ) were associated with isotropic hyperelasticity, I 4 and I 5 were involved with transversely isotropic hyperelasticity, I 6 to I 8 were concerned with isotropic magneto-mechanical behavior, and the last two were concerned with anisotropic magneto mechanical behavior. [150,152] As some of the strain invariants used in modeling anisotropic MREs have no physical meaning, several studies have been conducted in order to obtain mathematical relations in terms of a novel set of invariants that have a physical interpretation. The ability to design experimental setups for obtaining the material's constant parameters can be greatly improved by knowing the physical meaning of invariants.…”
Section: Continuum-based Modelsmentioning
confidence: 99%
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“…Many different kinds of MAE materials have been reported in the past couple of years. From the point of driving principle, MAE materials can be simply divided into two main categories (Beheshti et al, 2021; Lockette et al, 2011): Hard-magnetic-particle based MAE (H-MAE) and Soft-magnetic-particle based MAE (S-MAE), in which the latter can also be classified into Isotropic S-MAE and Anisotropic S-MAE. H-MAE with different geometric conditions can generate motions such as jump, swim, and wriggle under applied magnetic fields (Hu et al, 2018; Lum et al, 2016).…”
Section: Introductionmentioning
confidence: 99%