Magnetorheological Elastomer Composites: Modeling and Dynamic Finite Element Analysis

Magnetorheological Elastomer Composites: Modeling and Dynamic Finite Element Analysis

Delft University of Technology Magnetorheological elastomer composites Modeling and dynamic finite element analysis Yarali, Ebrahim; Ali Farajzadeh, Mohammad; Noroozi, Reza; Dabbagh, Ali; Khoshgoftar, Mohammad J.; Mirzaali Mazandarani, M. DOI 10.1016/j.compstruct.2020.112881 10.1016/j.compstruct.2020.113063 Publication date 2020 Document Version Final published version Published in Composite Structures Citation (APA) Yarali, E., Ali Farajzadeh, M., Noroozi, R., Dabbagh, A., Khoshgoftar, M. J., & Mirzaali Mazandarani, M. (2020). Magnetorheological elastomer composites: Modeling and dynamic finite element analysis. Composite Structures, 254, [112881]. https://doi.org/10.1016/j.compstruct.2020.112881, https://doi.org/10.1016/j.compstruct.2020.113063 Important note To cite this publication, please use the final published version (if applicable). Please check the document version above. Copyright Other than for strictly personal use, it is not permitted to download, forward or distribute the text or part of it, without the consent of the author(s) and/or copyright holder(s), unless the work is under an open content license such as Creative Commons. Takedown policy Please contact us and provide details if you believe this document breaches copyrights. We will remove access to the work immediately and investigate your claim. This work is downloaded from Delft University of Technology. For technical reasons the number of authors shown on this cover page is limited to a maximum of 10. Composite Structures 254 (2020) 112881 Contents lists available at ScienceDirect Composite Structures journal homepage: www.elsevier.com/locate/compstruct Magnetorheological elastomer composites: Modeling and dynamic finite element analysis Ebrahim Yarali a, Mohammad Ali Farajzadeh a, Reza Noroozi a, Ali Dabbagh a, Mohammad J. Khoshgoftar b, ⇑ Mohammad J. Mirzaali c, a School of Mechanical Engineering, College of Engineering, University of Tehran, Tehran 11155-4563, Iran b Department of Mechanical Engineering, Faculty of Engineering, Arak University, Arak 38156-88349, Iran c Department of Biomechanical Engineering, Faculty of Mechanical, Maritime, and Materials Engineering, Delft University of Technology (TU Delft), Mekelweg 2, 2628 CD Delft, The Netherlands ARTICLE INFO ABSTRACT Keywords: Magnetorheological elastomers (MREs) are polymers reinforced by ferromagnetic particles that show mag- Magnetorheological elastomers (MREs) netic dependent behavior. Mixing MREs with reinforcing fibers can create a new class of material so‐ Fiber‐reinforced composites (FRCs) called “MRE composites, MRECs” with additional functionalities and properties. Here, using a Generalized Finite element method (FEM) Maxwell model, we proposed a new magnetic‐dependent rheological model by considering the hysteresis First‐order shear deformation theory (FSDT) phenomenon for MREs to predict the dynamic damping responses of MREC plates reinforced by fibers in the frequency domain. We also investigated the influence of magnetic flux intensity, the volume fraction of the fiber, the orientation angle of the fibers, the number of layers, as well as the fiber‐to‐matrix stiffness ratio on the natural frequency, loss factor, and mode shapes of MRECs plates. Our results suggest that homogenously increasing the elastic properties of the MRECs through the spatial distribution of fibers and changing the fiber‐to‐matrix stiffness ratio can effectively tailor the dynamic properties of MRECs. Tailoring these properties can provide additional freedom for the fabrication of 4D‐printed MRE‐based composites. 1. Introduction netic or electric dependent behavior [8–14,67]. Among these smart materials, MR elastomers (MREs), which are polymers reinforced by Composite materials with superior material properties and func- ferromagnetic particles [15], have recently gained a great deal of tionalities are the results of the precise placement of their constituents, attention due to their sensitivity to the magnetic fields [16]. MREs namely fiber and matrix [1,2]. Examples are carbon fiber reinforced can be used as base materials in 3D printing processes [17], to create concretes with high tensile properties (i.e., low weight‐to‐strength structures with piezoresistivity [18], positive piezoconductivity [19], ratio with remarkable stiffness properties, high flexural strength or and adaptive mounting [20] capabilities. Having ferromagnetic parti- toughness [3]), functionally graded composites with improved interfa- cles, MREs can be polarized in specific directions parallel to the longi- cial bending strength and their stability investigations [4] and high tudinal direction of the magnetic field, which can eventually lead to a thermomechanical behavior [5], multi‐layer composites including hardening phenomenon [15]. Therefore, MREs can exhibit magneto‐ smart cores with excellent dynamic properties [6], and carbon fiber elastic interactions in the presence of damping behaviors. The dependency composites with damping enhancement [7]. of MREs on the magnetic field makes them useful to control the properties The advanced composite materials can be fabricated from smart ofmaterialsbymerelychangingtheexternalstimuli(e.g., the amplitude or materials such as shape memory alloys (SMAs), shape memory poly- direction of the magnetic field). Being activated by an external stimulus mers (SMPs), piezoelectrics, magneto‐electro‐elastics (MEE), elec- makes MREs an appropriate candidate for 4D printing where a shape‐ trorheological (ER) and magnetorheological (MR) materials. Using shifting of a 3D printed structure under external stimuli overtime is needed these materials can provide additional functionalities to the compos- [21–24]. Besides, tuning the elastic properties of MRE composites ites, such as shape memory effect, reversible cyclic behavior, and mag- (MRECs) provides an excellent opportunity to create materials with func- ⇑ Corresponding author. E-mail address: [email protected] (M.J. Mirzaali). https://doi.org/10.1016/j.compstruct.2020.112881 Received 7 January 2020; Revised 21 July 2020; Accepted 24 August 2020 Available online 28 August 2020 0263-8223/© 2020 The Authors. Published by Elsevier Ltd. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). E. Yarali et al. Composite Structures 254 (2020) 112881 tionally graded stiffnesses useful for several high‐tech industries such as We found the parameters of the proposed model in terms of the mag- biomedical or automotive industries. netic flux intensity obtained by a nonlinear regularization technique MREs were first used to test the dynamic characteristics of tunable fitted on the experimental DMA reported in the literature [26]. More- adaptive vibration absorbers [25]. The damping properties of polymer‐ over, the hysteresis behavior of the MRE composites in different fre- based composites in general and MRECs, in particular, can be influ- quencies and magnetic flux intensities were investigated within the enced by dynamic losses. The fabrication process and consequently framework of the developed model. Then, based on the the first‐ the damping response of MRECs can be optimized with respect to order shear deformation theory (FSDT), the formulation of the free the influences of various parameters, including the magnetic flux vibrational analysis of MRE‐based composite plates derived and solved intensity [26], the volume fraction of the magnetic particles, the orien- using finite elemenet (FE) approach. Also, the verification of the prob- tation of the particles, and material properties of the matrix (e.g., using lem was performed by comparison of FE code and those of commercial natural rubber as the matrix [27]). The damping phenomenon can be software (i.e., ABAQUS). We also parametrically analyzed the effect of started from the matrix, fiber, or from the interphase between the the magnetic field magnitude, fiber orientation and volume fraction, matrix and fiber [28]. Therefore, the spatial distribution and direction and elastic properties of fibers on the free vibration behavior of the of magnetic particles (i.e., isotropic or anisotropic orientations) in the MREC plates. MRECs can also tune the damping properties [29]. For example, it has been shown that anisotropic MREs exhibit higher modulus degrada- 2. Problem definition tion than those with isotropic particle distribution [27,29]. In the past, several computational and experimental studies have In this study, we assumed thin MRE‐based multi‐layer composite been performed on the vibrational [30], damping [31,32], dynamic plates. Therefore, to derive their constitutive equations, we used the stability [33,34], non‐linear static [35], and torsional dynamic [36] equivalent single layer (ESL) approach combined with the FSDT of responses and viscoelastic behavior [37] of composites with an MRE plates [50–53]. core. In addition, different phenomenological models have been pro- posed to simulate the magneto‐mechanical characteristics of MREs 2.1. Governing equations of multi-layer MREC plates [38–44] where various theoretical models for predicting the magnetic field‐dependent mechanical properties were used. Besides, MREs have We assumed that the multi‐layer composite plate consisted of n lay- applications in the fabrication of isolator devices where the effects of ers (Fig. 1a). Also, because of the negligible thickness of the plate in hysteresis are dominated. Several models have been proposed for such comparison with its length and width, the plane stress assumption applications

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