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Dispersion mechanism of nano-particulate aggregates using a high pressure wet-type jet mill

机译:高压湿式喷射磨分散纳米颗粒团聚体的机理

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A high pressure wet-type jet mill was employed to disperse nano-particle suspensions. Commercially available nano-particles, fumed silica (SiO2) of primary particle diameter (d(0)) ranging from 7 to 40 nm, alumina (Al2O3) of d(0) = 12 nm and titanium oxide (TiO2) of do = 21 nm were dispersed in the continuous phase up to viscosity eta(c) = 1000 mPa s. Ion exchanged water, aqueous ethylene glycol and aqueous polyethylene glycol solutions with molecular weight up to 2 000 000, were used as the continuous phase. Particle size distribution, zeta potential and suspension viscosity were measured under a wide range of process conditions. The smaller the do was, the harder it was to disperse the aggregates. Zeta potential was largely dependent on do at any process conditions and became dependent on eta(c) for eta(c) > 450 mPa s. The energy barrier was evaluated by taking van der Waals attractive forces, electrostatic repulsive forces and dispersive forces into consideration. Cavitation measurements showed a negligible cavitation during the passage through the jet mill; therefore aggregate disruption was modeled for fully turbulent flow. Aggregate disruption occurred in inertia sub-range for eta(c) <= 300 mPa s and in viscous sub-range for eta(c) >= 450 mpa s. By balancing mechanical energy with turbulent disruptive energy, a mechanistic model was developed for each sub-range. The analysis of fractal dimensionality showed that nano-aggregates were made up by particle-particle collision in inertia sub-range and orthokinetic cluster-cluster collision in viscous sub-range. The rheological data obtained were expressed according to a modified Casson model. (c) 2008 Elsevier Ltd. All rights reserved.
机译:使用高压湿式喷射磨机分散纳米颗粒悬浮液。市售纳米粒子,一次粒径(d(0))为7至40 nm的气相二氧化硅(SiO2),d(0)= 12 nm的氧化铝(Al2O3)和do = 21的二氧化钛(TiO2) nm分散在连续相中,直到粘度eta(c)= 1000 mPa s。离子交换水,乙二醇水溶液和分子量高达2000000的聚乙二醇水溶液被用作连续相。在广泛的工艺条件下测量粒度分布,ζ电位和悬浮液粘度。尺寸越小,分散骨料的难度就越大。 Zeta电位在任何工艺条件下都主要取决于do,对于eta(c)> 450 mPa s则取决于eta(c)。通过考虑范德华力,静电排斥力和分散力来评估能垒。空化测量表明,在通过喷射磨机的过程中,空化几乎可以忽略不计;因此,对总扰动建模为完全湍流。在eta(c)<= 300 mPa s的惯性子范围和eta(c)> = 450 mpa s的粘性子范围中发生聚集破坏。通过平衡机械能和湍流破坏能,为每个子范围开发了一种机械模型。分形维数分析表明,纳米聚集体是由惯性子范围内的颗粒-颗粒碰撞和粘性子范围内的正动力学簇-簇碰撞组成的。根据改进的Casson模型表示获得的流变数据。 (c)2008 Elsevier Ltd.保留所有权利。

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