共查询到16条相似文献,搜索用时 78 毫秒
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用接触角法测量聚合物共混体系的表面性能 总被引:11,自引:0,他引:11
利用接触角的方法研究了聚合物HDPF、PET及其共混物HDPE/PET的表面自由能、极化度以及与不同液体一水和甘油间界面张力的大小。 相似文献
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高度法和压力法测定粉末接触角的比较 总被引:2,自引:0,他引:2
粉体接触角的测定有着十分重要的理论和实际应用意义。根据Washburn方程,在渗透法测定粉末接触角的基础上,引入相对接触角的概念,并设计了测定石墨粉相对接触角的试验装置,以苯作为参比液,用高度法和压力法分别测定了25℃下蒸馏水对石墨粉的相对接触角,它们分别为83.50°和83.74°。试验结果表明,压力法和高度法均可用于粉末接触角的测定。 相似文献
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探讨了5种标准灭菌方法对3种硅表面涂层的影响:聚乙二醇(PEG)、聚甲基丙烯酸磺基甜菜碱(pSBMA)和聚2-甲基丙烯酰氧乙基磷酰胆碱(pMPC)。对高压釜、干热、过氧化氢(H2O2)等离子体、环氧乙烷气体(EtO)和电子束(E-beam)处理的涂层进行分析,以确定聚合物在灭菌过程中可能发生的降解。灭菌后,接触角有显著变化,H2O2引起的最大变化Δ-PEG、pSBMA和pMPC分别采用高压釜和干热处理。在PEG硅上使用高压釜和EtO,在pSBMA硅上使用电子束,在pMPC硅上使用EtO处理,发现涂层厚度变化小于5%。H2O2处理使所有涂层的厚度至少减少30%。酶联免疫吸附试验(ELISA)显示,在所有灭菌方法后,pMPC硅的蛋白质吸附量显著增加。PEG硅上的电子束和pSBMA硅上的干热处理在每个涂层子集中表现出最大的蛋白质吸附。总的来说,数据表明高压釜和EtO处理非常适合PEG硅,而E-beam最适合pSBMA硅。EtO处理对pMPC硅的影响最小。H 相似文献
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《高科技纤维与应用》2006,31(3):47
本发明提供含有以下成分(A)和成分(B),或成分(A’)、成分(B’)和成分(D)的碳纤维用上浆剂。成分(A):分子中含有1个或其以上环氧基,表面能为17~34mJ/m^2的环氧化合物、成分(B):分子中含有1个或其以上环氧基,表面能为35mJ/m^2或其以上的环氧化合物;成分(A’):分子小含有2个或其以上环氧基,表面能为17~34mJ/m^2的环氧化合物;成分(B’):分子中含有2个或其以上环氧基,表面能为35mJ/m^2或其以上的环氧化合物;以及成分(D):以铵离子作为对离子,以烯化氧加成量为10mol或其以下的芳氰基作为疏水基的阴离子表面活性剂。 相似文献
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The phenomenon of hysteresis of contact angle is an important topic subject to a long time of argument.A simple hydrostatic model of sessile drops under the gravity in combination with an ideal surface roughness model is used to interpret the process of drop volume increase or decrease of a planar sessile drop and to shed light on the contact angle hysteresis and its relationship with the solid surface roughness. With this model, the advancing and receding contact angles are conceptually explained in terms of equilibrium contact angle and surface roughness only,without invoking the thermodynamic multiplicity. The model is found to be qualitatively consistent to experimental observations on contact angle hysteresis and it suggests a possible way to approach the hysteresis of three-dimensional sessile drops. 相似文献
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Alain Carre 《The Journal of Adhesion》1995,54(1):167-174
A modified drop shape method has been developed to allow the simple determination of the surface free energy of a mineral glass. Our approach is based on the study of the profile of a large sessile drop of glass. The drop is formed by heating a glass cylinder settled on a horizontal solid plane.
The experimental parameters, in particular the size of the glass drop, leading to the accurate characterization of the surface free energy, have been determined by using mercury as a model of a high surface free energy liquid. It has been shown that the ratio between the diameter of the drop and the capillary length, (γ/ρμ)1/2, must be of the order of 10.
In this paper, practical details and results of measurements are presented for a series of four different glasses. A clear relationship between glass composition and surface free energy is observed. In particular, tin oxide reduces significantly the surface free energy of zinc phosphate glass. The coalescence of glass particles is probably related to glass surface and glass/polymer interfacial free energies. A discussion on how this may impact glass/polymer blend processability is presented. 相似文献
The experimental parameters, in particular the size of the glass drop, leading to the accurate characterization of the surface free energy, have been determined by using mercury as a model of a high surface free energy liquid. It has been shown that the ratio between the diameter of the drop and the capillary length, (γ/ρμ)1/2, must be of the order of 10.
In this paper, practical details and results of measurements are presented for a series of four different glasses. A clear relationship between glass composition and surface free energy is observed. In particular, tin oxide reduces significantly the surface free energy of zinc phosphate glass. The coalescence of glass particles is probably related to glass surface and glass/polymer interfacial free energies. A discussion on how this may impact glass/polymer blend processability is presented. 相似文献
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Observation and measurement were conducted to investigate contact angle and its hysteresis on rough surface. The experimental results indicate that the increase in solid surface roughness enlarges advancing contact angle and decreases receding contact angle, resulting in enhanced hysteresis. It was observed that when Young's contact angle θY < 90°, as the roughness of solid surface increased the extent of the decrease in 相似文献
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Jaroslaw Drelich 《The Journal of Adhesion》1997,63(1):31-51
Examples of experimental contact angle data for varying drop and bubble volumes on different solids whose surfaces are smooth and homogeneous, rough and homogeneous, smooth and heterogeneous, and covered with unstable organic films are presented. The ideas and theoretical models as proposed in the literature for the interpretation of contact angle/drop (bubble) size relationships are critically reviewed. It is shown that major factors affecting the contact angle variation with drop (bubble) size such as surface heterogeneity, roughness, and stability, have been identified in the literature. However, there is still a need for experimental work with well-defined and well-characterized solid surfaces. Theoretical models that have been proposed in the literature are still inadequate. Advanced modeling of liquid behavior at heterogeneous and rough surfaces is required to understand further, and to predict, the contact angle/drop (bubble) size relationships at imperfect surfaces. 相似文献
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Jaroslaw Drelich 《The Journal of Adhesion》2013,89(1-3):31-51
Examples of experimental contact angle data for varying drop and bubble volumes on different solids whose surfaces are smooth and homogeneous, rough and homogeneous, smooth and heterogeneous, and covered with unstable organic films are presented. The ideas and theoretical models as proposed in the literature for the interpretation of contact angle/drop (bubble) size relationships are critically reviewed. It is shown that major factors affecting the contact angle variation with drop (bubble) size such as surface heterogeneity, roughness, and stability, have been identified in the literature. However, there is still a need for experimental work with well-defined and well-characterized solid surfaces. Theoretical models that have been proposed in the literature are still inadequate. Advanced modeling of liquid behavior at heterogeneous and rough surfaces is required to understand further, and to predict, the contact angle/drop (bubble) size relationships at imperfect surfaces. 相似文献
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