Abstract

The interaction of an external magnetic field with magnetic objects affects their response and is a fundamental property for many biomedical applications, including magnetic resonance and particle imaging, electromagnetic hyperthermia, and magnetic targeting and separation. Magnetic alignment and relaxation are widely studied in the context of these applications. In this study, we theoretically investigate the alignment dynamics of a rotational magnetic particle as an inverse process to Brownian relaxation. The selected external magnetic flux density ranges from 5μT to 5T. We found that the viscous torque for arbitrary rotating particles with a history term due to the inertia and friction of the surrounding ambient water has a significant effect in strong magnetic fields (range 1–5T). In this range, oscillatory behavior due to the inertial torque of the particle also occurs, and the stochastic Brownian torque diminishes. In contrast, for weak fields (range 5–50μT), the history term of the viscous torque and the inertial torque can be neglected, and the stochastic Brownian torque induced by random collisions of the surrounding fluid molecules becomes dominant. These results contribute to a better understanding of the molecular mechanisms of magnetic particle alignment in external magnetic fields and have important implications in a variety of biomedical applications.

Highlights

  • When subjected to an external magnetic field, a magnetic particle will respond with translational motion in the gradient magnetic field and its self-rotation, or rotation of its magnetic moment, to the direction of the external magnetic field as it is applied in various cases of biomedical applications widely studied experimentally and theoretically [1,2,3,4,5,6,7,8,9,10]

  • These latter effects are denoted as magnetic alignment and are inverse processes to Brownian and Néel relaxation [11,12]

  • Magnetic particle alignment at the nano- and micro-scale requires a complex approach for simulating a wide range of possible strengths of an acting external magnetic field

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Summary

Introduction

When subjected to an external magnetic field, a magnetic particle will respond with translational motion in the gradient magnetic field and its self-rotation, or rotation of its magnetic moment, to the direction of the external magnetic field as it is applied in various cases of biomedical applications widely studied experimentally and theoretically [1,2,3,4,5,6,7,8,9,10] These latter effects are denoted as magnetic alignment and are inverse processes to Brownian and Néel relaxation [11,12]. If we restrict only the particle rotating (as a whole with a magnetic moment) to the direction of an external homogeneous magnetic field, the particle experiences a magnetic torque that can be described analytically [28]

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