Makarova Liudmila A, Isaev Danil A, Omelyanchik Alexander S, Alekhina Iuliia A, Isaenko Matvey B, Rodionova Valeria V, Raikher Yuriy L, Perov Nikolai S
Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia.
Institute of Physics, Mathematics & IT, Immanuel Kant Baltic Federal University, 236041 Kaliningrad, Russia.
Polymers (Basel). 2021 Dec 31;14(1):153. doi: 10.3390/polym14010153.
Multiferroics are materials that electrically polarize when subjected to a magnetic field and magnetize under the action of an electric field. In composites, the multiferroic effect is achieved by mixing of ferromagnetic (FM) and ferroelectric (FE) particles. The FM particles are prone to magnetostriction (field-induced deformation), whereas the FE particles display piezoelectricity (electrically polarize under mechanical stress). In solid composites, where the FM and FE grains are in tight contact, the combination of these effects directly leads to multiferroic behavior. In the present work, we considered the FM/FE composites with soft polymer bases, where the particles of alternative kinds are remote from one another. In these systems, the multiferroic coupling is different and more complicated in comparison with the solid ones as it is essentially mediated by an electromagnetically neutral matrix. When either of the fields, magnetic or electric, acts on the 'akin' particles (FM or FE) it causes their displacement and by that perturbs the particle elastic environments. The induced mechanical stresses spread over the matrix and inevitably affect the particles of an alternative kind. Therefore, magnetization causes an electric response (due to the piezoeffect in FE) whereas electric polarization might entail a magnetic response (due to the magnetostriction effect in FM). A numerical model accounting for the multiferroic behavior of a polymer composite of the above-described type is proposed and confirmed experimentally on a polymer-based dispersion of iron and lead zirconate micron-size particles.
多铁性材料是指在磁场作用下发生电极化、在电场作用下产生磁化的材料。在复合材料中,多铁性效应是通过混合铁磁(FM)和铁电(FE)颗粒来实现的。FM颗粒易于发生磁致伸缩(场致变形),而FE颗粒表现出压电性(在机械应力下发生电极化)。在FM和FE晶粒紧密接触的固体复合材料中,这些效应的结合直接导致多铁性行为。在本工作中,我们考虑了以软聚合物为基体的FM/FE复合材料,其中不同种类的颗粒彼此远离。在这些系统中,与固体复合材料相比,多铁性耦合不同且更为复杂,因为它本质上是由电磁中性的基体介导的。当磁场或电场作用于“同类”颗粒(FM或FE)时,会导致它们发生位移,从而扰乱颗粒的弹性环境。由此产生的机械应力会在基体中传播,并不可避免地影响另一种颗粒。因此,磁化会引起电响应(由于FE中的压电效应),而电极化可能会引发磁响应(由于FM中的磁致伸缩效应)。本文提出了一个考虑上述类型聚合物复合材料多铁性行为的数值模型,并在基于聚合物的铁和锆酸铅微米级颗粒分散体上进行了实验验证。