摘要
因为磁性液体的磁性微粒有着很强的相互作用,Langevin顺磁理论不能很好描述磁性液体的磁化强度随外磁场的变化.研究认为影响磁化的主要因素是磁性液体内微粒整体的结构化,其结构的形成储存了部分磁化功,直接或间接地影响了磁化.在此基础上提出“压缩”模型,修正了描述磁性液体常用的Langevin函数,得出了与实验较好符合的曲线.所提出的一个压缩后等效体积分数与外磁场强度的关系式,近似地描述了磁性液体在磁场中磁化的过程.由修正式得出了近似初始磁化率随体积分数变化关系.
The Langevin paramagnetic theory can't describe the relation between magnetization of ferrofluids and applied magnetic field. The structuralization of ferrofluids, which is considered the main influence factor of the magnetization, is regarded. The part of magnetization works is deposited when the structure is forming. This action influences the magnetization of ferrofluids directly or indirectly. On the base of the “compressing” model, the Langevin function that usually describes the magnetization of ferrofluid is modified, and a well-fitted curve is obtained. An equation of the relation between the equivalent volume fraction after being “compressed” and the intensity of magnetic field is discovered, which approximately describes the process of magnetization. The relation between the approximate initial susceptibility and the volume fraction can be obtained from modified formula.
基金
ProjectsupportedbytheFundofNaturalScienceofChongqingCity
关键词
自形成
磁性液体
磁化特性
结构
熵
Self-formed, Ferrofluid, Magnetization, Structure, Entropy