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Study of the effect of dipole interactions on hyperthermia heating the cluster composed of superparamagnetic nanoparticles

机译:偶极相互作用对高温加热超顺磁性纳米粒子簇的影响研究

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In the present work, we investigate the effect of dipole interactions on hyperthermia heating the cluster composed of multi superparamagnetic nanoparticles via time-quantified Monte Carlo simulation. The dynamic hysteresis loop area of non-interacting particles calculated by a modified Rosensweig’s model is shown to be proportional to the field frequency. The inverse of the total number of Monte Carlo steps per field cycle is considered as a computational frequency in our modelling. By comparing the two proportionality constants gained from the simulation and from the Rosensweig’s model, respectively, the time scale of one Monte Carlo step is estimated. The shape of the cluster is characterised by treating it as an equivalent ellipsoid. When the morphology of cluster is highly anisotropic such in a chain and cylinder, dipole interactions align the moments of the particles to the morphology anisotropy axis of the cluster. The strength of such alignment depends on the magnitude of morphology anisotropy of the cluster. The alignment helps improve heating capability of the chain and cylinder clusters at the most angles between the field direction and morphology anisotropy axis. However, when the field direction is away from the axis too much, the high energy barrier will hamper the cluster to maintain the magnetization, leading to a reduced heating efficiency. Once the cluster loses its morphology anisotropy (i.e. cube), the influence of dipole interactions on hysteresis losses is reduced to the minimum; the probability to obtain an improved heating becomes very low no matter with the type of particle arrangement.
机译:在目前的工作中,我们通过时间量化的蒙特卡洛模拟研究了偶极子相互作用对热疗加热由多个超顺磁性纳米粒子组成的团簇的影响。修改后的Rosensweig模型计算出的非相互作用粒子的动态磁滞回线面积与磁场频率成正比。每个场周期的蒙特卡洛步数总数的倒数在我们的建模中被视为计算频率。通过比较分别从仿真和Rosensweig模型获得的两个比例常数,可以估算出一个蒙特卡洛步长的时间尺度。团簇的形状通过将其视为等效椭圆体来表征。当团簇的形态在链和圆柱中呈高度各向异性时,偶极相互作用将粒子的矩对准团簇的形态各向异性轴。这种排列的强度取决于簇的形态各向异性的大小。对准有助于在场方向和形态各向异性轴之间的最大角度处提高链和圆柱团簇的加热能力。但是,当磁场方向离轴太远时,高能垒将妨碍簇保持磁化强度,从而导致加热效率降低。一旦团簇失去其形态各向异性(即立方体),偶极相互作用对磁滞损耗的影响就减小到最小。无论粒子排列的类型如何,获得改善的加热的可能性都变得非常低。

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