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不同形状因子的粘土的防潮层涂层的振荡剪切响应。

Oscillatory shear response of moisture barrier coatings containing clay of different shape factor.

机构信息

CSIRO Materials Science and Engineering, Clayton South MDC, VIC, Australia.

出版信息

J Colloid Interface Sci. 2011 Jun 1;358(1):25-31. doi: 10.1016/j.jcis.2011.02.051. Epub 2011 Feb 24.

Abstract

Oscillatory shear rheology of barrier coatings based on dispersed styrene-butadiene latex and clay of various shape factors or aspect ratio has been explored. Barrier performance of these coatings when applied to paperboard has been assessed in terms of water vapour transmission rates and the results related to shape factor, dewatering and critical strain. It has been shown that a system based on clay with high shape factor gives a lower critical strain, dewatering and water vapour transmission rate compared with clays of lower shape factor. The dissipated energy, as calculated from an amplitude sweep, indicated no attractive interaction between clay and latex implying a critical strain that appears to be solely dependent on the shape factor at a constant volume fraction. Particle size distribution was shown to have no effect on the critical strain while coatings of high elasticity exhibited high yield strains as expected. The loss modulus demonstrated strain hardening before the elastic to viscous transition. The loss modulus peak was identified by a maximum strain which was significantly lower for a coating based on clay with a high shape factor. The characteristic elastic time was found to vary between 0.6 and 1.3s. The zero shear viscosity of barrier dispersion coatings were estimated from the characteristic elastic time and the characteristic modulus to be of the order of 25-100 Pa s.

摘要

已经研究了基于分散的苯乙烯-丁二烯胶乳和不同形状因子或纵横比的粘土的阻隔涂层的振荡剪切流变学。通过水蒸气透过率评估了这些涂层应用于纸板时的阻隔性能,并将结果与形状因子、脱水和临界应变相关联。结果表明,与形状因子较低的粘土相比,基于高形状因子粘土的体系具有较低的临界应变、脱水和水蒸气透过率。从振幅扫描计算出的耗散能表明粘土和胶乳之间没有吸引力相互作用,这意味着在恒定体积分数下,临界应变似乎仅取决于形状因子。粒径分布对临界应变没有影响,而高弹性的涂层表现出高屈服应变,这是预期的。在弹性向粘性转变之前,损耗模量表现出应变硬化。损耗模量峰值通过最大应变来识别,对于基于高形状因子粘土的涂层,最大应变明显更低。发现特征弹性时间在 0.6 和 1.3s 之间变化。从特征弹性时间和特征模量估算阻隔分散涂层的零剪切粘度约为 25-100Pa·s。

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