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首页> 外文期刊>Chemical Engineering Communications >An Invariant General Solution for the Magnetic Fields within and Surrounding a Small Spherical Particle in an Imposed Arbitrary Magnetic Field and the Resulting Magnetic Force and Couple
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An Invariant General Solution for the Magnetic Fields within and Surrounding a Small Spherical Particle in an Imposed Arbitrary Magnetic Field and the Resulting Magnetic Force and Couple

机译:施加于任意磁场中的小球形粒子内部和周围的磁场的不变一般解,以及由此产生的磁力和耦合

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摘要

A general coordinate-system invariant solution for the magnetic field and flux density within and surrounding a spherical particle in a linearly magnetizable medium in an arbitrary, externally applied field is developed for cases where the particle possesess homogeneous permanent and/or linear magnetization. The solution is consistent with the equations of magnetostatics and asymptotically exact in a regular perturbation sense, where the expansion parameter is the ratio of particle radius a to characteristic length scale L for variations in the externally applied field. Expressions for the magnetic field and flux, accurate to O(a/L), are used to determine the magnetic force and couple exerted on the particle by integration of the Maxwell stress tensor over the particle surface. This result is shown to be the same for some of the various reported expressions for the magnetic body force density (e.g., the Kelvin, Helmholtz, and Korteweg-Helmholtz) and is consistent with previously derived expressions for the magnetic force. It is further shown that the effective dipole method yields results consistent with these calculations. The results may be applied to the analogous electrostatic situation by replacing the magnetic quantities by their electric analogues.
机译:针对粒子具有均匀永久磁化和/或线性磁化的情况,针对在可线性磁化介质中的球形粒子内部及其周围的磁场和通量密度,在任意外部施加的磁场中,开发了一种通用的坐标系不变解。该解决方案与常规静力学意义上的静磁方程和渐近精确方程一致,其中膨胀参数是颗粒半径a与特征长度标度L的比值,用于外部施加磁场的变化。精确到O(a / L)的磁场和磁通表达式用于确定磁力和通过粒子表面上Maxwell应力张量的积分对施加在粒子上的耦合。对于磁力强度密度的各种报告表达式中的某些表达式(例如开尔文,亥姆霍兹和科特维格-亥姆霍兹),该结果显示出相同的结果,并且与先前推导的磁力表达式是一致的。进一步表明,有效偶极法得出的结果与这些计算结果一致。通过用其电模拟物代替磁量,可以将结果应用于类似的静电情况。

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