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首页> 外文期刊>Langmuir: The ACS Journal of Surfaces and Colloids >Interaction forces in thin liquid films stabilized by hydrophobically modified inulin polymeric surfactant. 1. Foam films
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Interaction forces in thin liquid films stabilized by hydrophobically modified inulin polymeric surfactant. 1. Foam films

机译:疏水改性的菊粉聚合物表面活性剂稳定的液体薄膜中的相互作用力。 1.泡沫膜

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Using the interferometric method of Scheludko-Exerowa for investigation of foam films, we have obtained results using a hydrophobically modified inulin polymeric surfactant (INUTEC SP1). Measurements were carried out at constant INUTEC SP1 concentration of 2 x 10(-5) mol(.)dm(-3) and at various NaCl concentrations ( in the range 1 x 10(-4) to 2 mol(.)dm(-3)). At constant capillary pressure of 50 Pa, the film thickness decreased gradually with an increase in NaCl concentration up to 10(-2) mol(.)dm(-3) NaCl above which the film thickness remains virtually constant at about 16 nm. This reduction in film thickness with an increase in NaCl concentration is due to the compression of the double layer and at the critical electrolyte concentration (C-el,C-cr = 10(-2) mol(.)dm(-3)) the electrostatic component of the disjoining pressure is completely screened and the remaining pressure is due to the steric interaction between the adsorbed polymer layers. Disjoining pressure-thickness (Pi-h) isotherms were obtained at C-el < C-el,C-cr (10(-4)-10(-3) mol(.)dm(-3)) and C-el > C-el,C-cr (0.5, 1, and 2 mol(.)dm(-3)). In the first case, the disjoining pressure isotherms could be fitted using the classical DLVO theory, Pi = Pi(el) + Pi(vw), and using the constant charge model. At C-el > C-el,C-cr, the main repulsion is due to the steric interaction between the polyfructose loops that exist at the air-water interface, i.e., Pi = Pi(st) + Pi(vw). Under these conditions, there is a sharp transition from DLVO to non-DLVO forces. In the latter case, the interaction could be described using the de Gennes' scaling theory. This gave an adsorbed layer thickness of 6.5 nm which is in reasonable agreement with the values obtained at the solid-solution interface. The (Pi-h) isotherms showed that these foam films are not very stable and they tend to collapse above a critical capillary pressure (of about 1 x 103 Pa), and these results could be used to predict the foam stability.
机译:使用Scheludko-Exerowa的干涉法研究泡沫膜,我们使用疏水改性的菊粉聚合物表面活性剂(INUTEC SP1)获得了结果。在恒定的INUTEC SP1浓度为2 x 10(-5)mol(。)dm(-3)和各种NaCl浓度(范围为1 x 10(-4)至2 mol(。)dm( -3))。在50 Pa的恒定毛细管压力下,随着NaCl浓度的增加,膜厚度逐渐减小,直至达到10(-2)mol(。)dm(-3)NaCl,在此之上,膜厚度实际上保持恒定在约16 nm。随着NaCl浓度的增加,膜厚度的减小是由于双层的压缩和临界电解质浓度所致(C-el,C-cr = 10(-2)mol(。)dm(-3))。分离压力的静电成分被完全屏蔽,剩余压力归因于吸附的聚合物层之间的空间相互作用。在C-el C-el,C-cr(0.5、1和2 mol(。)dm(-3)。在第一种情况下,可以使用经典的DLVO理论拟合Pi = Pi(el)+ Pi(vw),并使用恒定电荷模型拟合分离的等温线。在C-el> C-el,C-cr时,主要排斥是由于存在于空气-水界面的多聚果糖环之间的空间相互作用,即Pi = Pi(st)+ Pi(vw)。在这种情况下,从DLVO到非DLVO的部队将急剧过渡。在后一种情况下,可以使用de Gennes的缩放理论描述相互作用。得到的吸附层厚度为6.5nm,与在固溶界面处获得的值合理地吻合。 (Pi-h)等温线表明,这些泡沫膜不是很稳定,在高于临界毛细管压力(约1 x 103 Pa)时它们往往会塌陷,这些结果可用于预测泡沫的稳定性。

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