Mostarac Deniz, Sánchez Pedro A, Kantorovich Sofia
University of Vienna, Vienna, Austria.
Ural Federal University, Ekaterinburg, Russia and Wolfgang Pauli Institute, Vienna, Austria.
Nanoscale. 2020 Jul 9;12(26):13933-13947. doi: 10.1039/d0nr01646b.
Incorporating magnetic nanoparticles (MNPs) within permanently crosslinked polymer-like structures opens up the possibility for synthesis of complex, highly magneto-responsive systems. Among such structures are chains of prealigned magnetic (ferro- or super-paramagnetic) monomers, permanently crosslinked by means of macromolecules, which we refer to as magnetic filaments (MFs). In this paper, using molecular dynamics simulations, we encompass filament synthesis scenarios, with a compact set of easily tuneable computational models, where we consider two distinct crosslinking approaches, for both ferromagnetic and super-paramagnetic monomers. We characterise the equilibrium structure, correlations and magnetic properties of MFs in static magnetic fields. Calculations show that MFs with ferromagnetic MNPs in crosslinking scenarios where the dipole moment orientations are decoupled from the filament backbone, have similar properties to MFs with super-paramagnetic monomers. At the same time, magnetic properties of MFs with ferromagnetic MNPs are more dependent on the crosslinking approach than they are for ones with super-paramagnetic monomers. Our results show that, in a strong applied field, MFs with super-paramagnetic MNPs have similar magnetic properties to ferromagnetic ones, while exhibiting higher susceptibility in low fields. We find that MFs with super-paramagnetic MNPs have a tendency to bend the backbone locally rather than to fully stretch along the field. We explain this behaviour by supplementing Flory theory with an explicit dipole-dipole interaction potential, with which we can take in to account folded filament configurations. It turns out that the entropy gain obtained through bending compensates an insignificant loss in dipolar energy for the filament lengths considered in the manuscript.
将磁性纳米颗粒(MNP)纳入永久交联的聚合物状结构中,为合成复杂的、高度磁响应系统开辟了可能性。在这类结构中,有通过大分子永久交联的预排列磁性(铁磁性或超顺磁性)单体链,我们将其称为磁丝(MF)。在本文中,我们使用分子动力学模拟,通过一组紧凑且易于调整的计算模型来研究丝的合成情况,其中我们考虑了两种不同的交联方法,用于铁磁和超顺磁单体。我们表征了静态磁场中MF的平衡结构、相关性和磁性。计算表明,在偶极矩取向与丝骨架解耦的交联情况下,含有铁磁MNP的MF具有与含有超顺磁单体的MF相似的性质。同时,含有铁磁MNP的MF的磁性比含有超顺磁单体的MF更依赖于交联方法。我们的结果表明,在强外加磁场中,含有超顺磁MNP的MF具有与铁磁MF相似的磁性,而在低场中表现出更高的磁化率。我们发现,含有超顺磁MNP的MF倾向于使骨架局部弯曲,而不是沿磁场完全伸展。我们通过用明确的偶极 - 偶极相互作用势补充弗洛里理论来解释这种行为,利用该势我们可以考虑折叠丝的构型。结果表明,通过弯曲获得的熵增补偿了本文所考虑的丝长度下偶极能量的微小损失。