Barrie C L, Griffiths P C, Abbott R J, Grillo I, Kudryashov E, Smyth C
School of Chemistry, Cardiff University, P.O. Box 912, Cardiff CF10 3TB, UK.
J Colloid Interface Sci. 2004 Apr 1;272(1):210-7. doi: 10.1016/j.jcis.2003.12.004.
The interaction of carbon black with an acrylic resin has been investigated by rheology. Two carbon blacks, with similar particle size and surface characteristics but quite different particle morphologies, have been examined. These are somewhat arbitrarily denoted as "spherical" and "fractal" as shown by small-angle neutron scattering (SANS) and ultrasonic spectroscopy studies. In the absence of polymer, stable aqueous dispersions could not be obtained. Stable dispersions could be obtained, however, upon addition of polymer to a level corresponding to a ratio of 50 mg of polymer per 13 m2 (+/- m2) of surface area (i.e., 15 wt% particles). These stable dispersions exhibit flow typical of concentrated dispersions-Newtonian behavior up to some apparent "yield" or critical value, above which pronounced shear thinning is observed. The critical stress increases with increasing polymer concentration. When a significant amount of nonadsorbed polymer is also present, a second Newtonian plateau is superimposed on the shear-thinning behavior. This feature is observed for both particle types but is more pronounced for the fractal particle. When there is little or no nonadsorbed polymer, the viscosity of the fractal particle dispersions is greater than the viscosity of the spherical particle dispersions. At low polymer concentrations, the dispersions are predominantly viscous at low shear stresses. The phase angle decreases significantly over a narrow shear stress range and the rheology tends to more elastic behavior. At higher shear stresses, the dependence on particle morphology is weak.
通过流变学研究了炭黑与丙烯酸树脂的相互作用。研究了两种炭黑,它们具有相似的粒径和表面特性,但颗粒形态却大不相同。如小角中子散射(SANS)和超声光谱研究所示,这两种炭黑有点随意地被标记为“球形”和“分形”。在没有聚合物的情况下,无法获得稳定的水分散体。然而,当聚合物添加到对应于每13平方米(±1平方米)表面积50毫克聚合物的比例(即15重量%颗粒)时,可以获得稳定的分散体。这些稳定的分散体表现出典型的浓分散体流动特性——在达到某个明显的“屈服”或临界值之前呈牛顿行为,超过该值则观察到明显的剪切变稀。临界应力随聚合物浓度的增加而增加。当还存在大量未吸附的聚合物时,在剪切变稀行为上叠加了第二个牛顿平台。两种颗粒类型都观察到了这一特征,但分形颗粒更为明显。当几乎没有或没有未吸附的聚合物时,分形颗粒分散体的粘度大于球形颗粒分散体的粘度。在低聚合物浓度下,分散体在低剪切应力下主要表现为粘性。相角在狭窄的剪切应力范围内显著减小,流变学倾向于更具弹性的行为。在较高的剪切应力下,对颗粒形态的依赖性较弱。