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Modeling the Brownian relaxation of nanoparticle ferrofluids: Comparison with experiment

机译:纳米铁磁流体的布朗弛豫建模:与实验的比较

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We obtain good agreement between the calculated and measured ratio of harmonics only when the model includes nanoparticles which have a distribution in the hydrodynamic diameter - that is polydisperse. We are unable to find good agreement if the diameter of the nanoparticles is constrained to only one value - that is monodisperse. In Fig. 1 we plot the measured [3] ratios of 5th/3rd harmonics of the magnetization for samples using “100 nm” iron oxide particles (top plot) and “40 nm” iron oxide particles (bottom plot). The measurements were collected with the nanoparticles in ferrofluid solutions with a range of water/glycerol ratios corresponding to different viscosities (and therefore different Brownian relaxation times.) As described in [3] the data are plotted as a function of ωτB. Also shown in Fig. 1 are the calculations of the ratios of 5th/3rd harmonics assuming both monodisperse and polydisperse ferrofluids. Details of the calculations and parameters used in the models can be found in [5].
机译:仅当模型包含在流体动力学直径中具有分布(即多分散)的纳米颗粒时,我们才能在计算出的谐波比和测量出的谐波比之间取得良好的一致性。如果将纳米颗粒的直径限制在一个值(单分散),我们将找不到很好的协议。在图1中,我们绘制了使用“ 100 nm”氧化铁颗粒的样品的磁化强度的5 / 3 rd 谐波的测量的[3]比率(上图)和“ 40 nm”氧化铁颗粒(下图)。用铁磁流体溶液中的纳米颗粒收集测量值,该纳米颗粒在一定范围内的水/甘油比对应于不同的粘度(因此也具有不同的布朗弛豫时间)。如[3]中所述,将数据绘制为ωτinf B的函数。图1还显示了假设单分散和多分散铁磁流体的5 / 3 rd 谐波比率的计算。模型中使用的计算和参数的详细信息可以在[5]中找到。

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