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University of Cambridge > Talks.cam > Engineering - Mechanics Colloquia Research Seminars > Soft elasticity by domain formation in reinforced and magneto-active composites
Soft elasticity by domain formation in reinforced and magneto-active compositesAdd to your list(s) Download to your calendar using vCal
If you have a question about this talk, please contact Hilde Hambro. Reinforced elastomeric composites with periodic microstructures can undergo both microscopic (pattern changing) and macroscopic (long wavelength) instabilities. This presentation is concerned with the response of magneto-active elastomeric composites after the possible development of a macroscopic instability, which have been previously characterized in terms of loss of strong ellipticity of the incremental homogenized response of the composite material and can also occur when the microstructures are random. Building on earlier work in the purely mechanical context, it is shown by means of a generalized Maxwell construction that the composite loses stability by the formation of lamellar domains, on a scale much larger than that of the fibers, and where the orientation of the fibers changes abruptly from domain to domain in a chevron-type pattern. Mathematically, this corresponds to the relaxation or quasiconvexification of the principal solution for the homogenized energy function and is associated with soft modes of deformation that can be controlled by externally applied magnetic fields. For analytical ease, we consider the application to simple laminate composites consisting of two isotropic neo-Hookean phases with linear magnetic responses and obtain estimates for the homogenized relaxed response under combined magneto-mechanical loadings. One important finding is that an externally applied magnetic field can be used to trigger the instability without the application of mechanical loads. Another very interesting finding is that there are perfectly soft modes of deformation where the deformation can be accommodated purely by appropriate changes in the domain microstructures — without changes in the applied stress. At the more theoretical level, it is found that strict global rank-one convexity of the principal solution is generally lost prior to local rank-one convexity, or strong ellipticity. This suggest a new definition of macroscopic instabilities in terms of loss of global rank-one convexity. This talk is part of the Engineering - Mechanics Colloquia Research Seminars series. This talk is included in these lists:
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