聚合物分散剂对氟铃脲水悬浮剂流变性质的影响

采用控制应力流变仪研究了聚合物分散剂苯乙烯丙烯酸无规共聚物（MOTAS）用量、分子量及氟铃脲质量分数等对氟铃脲水悬浮剂流变性质的影响。 结果表明,以聚合物MOTAS为分散剂制备的氟铃脲水悬浮剂的流变行为符合Herschel-Bulkley模型。 在固定氟铃脲质量分数为20%时,当分散剂质量分数≤3.0%时,流动行为指数n≤1.0,悬浮体系表现为假塑性流体,当分散剂质量分数≥3.5%时,流动行为指数n≥1.0,悬浮体系具有胀塑性流体特征。 氟铃脲水悬浮剂的流变参数屈服值τH与分散剂MOTAS和氟铃脲的加入量有关。 分散剂MOTAS质量分数≤2.5%时,分散剂在氟铃脲颗粒界面吸附很少,裸露的氟铃脲颗粒界面间相互搭接,具有较大的屈服值τH;当分散剂加入质量分数为3.0%时,分散剂可在氟铃脲颗粒界面形成饱和吸附,若再增加分散剂用量,多余分散剂在悬浮的氟铃脲颗粒间形成搭接,使其屈服值τH增大。 在MOTAS分散剂的分子量在10 000~30 000范围内时,MOTAS分子量愈大,所制得的氟铃脲水悬浮剂的表观粘度和屈服值τH愈小,流变行为指数n虽略有增加,但均小于1,没有改变“剪切变稀”的假塑性特征。     

溶剂替换法制备氟铃脲水悬浮剂及其分散稳定性

采用溶剂替换法制备了氟铃脲水悬浮剂,通过测定颗粒的平均粒径Dav和颗粒界面的Zeta电位,研究了分散剂种类、添加量以及有机相中乙醇的加入量对水悬浮剂分散稳定性的影响。 结果表明,在相同条件下,以苯乙烯丙烯酸共聚物(MOTAS)作为分散剂制备的水悬浮剂的分散效果较好;当MOTAS添加质量分数为1%时,Dav最小,Zeta电位绝对值最大,体系分散稳定性最好;在有机相中添加乙醇可以显著提高氟铃脲水悬浮剂的分散稳定性,当有机相中乙醇的加入质量分数增加至31.2%时分散稳定性达到最好。     

聚羧酸型梳状共聚物超分散剂在氟虫腈颗粒界面的吸附性能

采用紫外光谱(UV)、 傅里叶变换红外光谱(FTIR)、 X射线光电子能谱(XPS)和扫描电子显微镜(SEM)对聚羧酸型梳状共聚物超分散剂(TERSPERSE^®2700)在氟虫腈颗粒界面的吸附等温线、 吸附动力学、 吸附作用力、 吸附层厚度以及吸附状态等进行了分析. 实验结果表明, TERSPERSE^®2700分散剂在氟虫腈颗粒界面的吸附模型符合Langmuir吸附等温式, 吸附量随着温度升高而增大, 并计算了ΔG^0-, ΔH^0-和ΔS^0-. 吸附符合准一级动力学模型, 吸附速率常数随着温度升高而增大, 吸附活化能E_a=29.28 kJ/mol. 利用XPS谱图, 估算其吸附厚度约为1 nm, 表明存在吸附作用. 实验发现氟虫腈存在分子间氢键, 同时氢键也是分散剂分子与氟虫腈颗粒表面结合的重要作用力.     

木质素系和萘系分散剂在煤水界面的吸附性能

研究了两种木质素类分散剂SL(木质素磺酸钠)和MSSL(改性磺化碱木质素钠盐)和一种萘系分散剂(FDN)在大同煤表面的吸附量和动力学, 结果表明, SL和MSSL在煤表面的吸附量远比FDN的大, 但是拟合所得的Langmuir平衡常数K和吸附速率常数ka都比FDN的小, 这表明SL和MSSL在煤表面的吸附能力比FDN略差, 吸附速率较慢. 采用IR和XPS研究了煤表面分散剂吸附层的结果表明, 吸附了SL和MSSL的煤表面具有明显的“红移”现象, 并且SL和MSSL在煤表面的吸附层厚度分别为7.22和4.61 nm, 而FDN的吸附层厚度较小, 为2.11 nm. 分析认为, SL和MSSL在煤表面的吸附以氢键力为主, 吸附量较大, 吸附层较厚, 在煤表面呈多点式吸附; FDN主要以π电子极化吸附在煤表面呈卧式吸附, 吸附强度较大, 吸附层较薄.     

聚合物分散剂对氟虫脲水悬浮剂分散稳定性的影响

通过测定药物颗粒界面Zeta电位和平均粒径, 研究了聚合物分散剂苯乙烯磺酸聚合物钠盐(GY-D08)用量、pH和盐离子对氟虫脲水悬浮剂分散稳定性的影响, 研究结果表明, 分散剂GY-D08的加入量与水悬浮剂分散效果密切相关, 制备质量分数为5%氟虫脲水悬浮剂的GY-D08最佳用量为2%, GY-D08用量过多或过少都会使分散效果下降; pH影响分散剂GY-D08在水中的电离能力, 当pH=9时, GY-D08分子完全电离, 能为颗粒提供较大的静电位阻, 水悬浮剂分散稳定性最好; Mg²⁺或Ca²⁺压缩颗粒界面的双电层, 降低Zeta电位, 使颗粒因带电量减少而聚结, 导致水悬浮剂分散稳定性变差, 且Mg²⁺或Ca²⁺浓度愈大, 其分散稳定性愈差; 当离子浓度相同时, Ca²⁺压缩双电层的能力比Mg²⁺强, 添加Ca²⁺后的水悬浮剂的分散稳定性更差.     

聚丙烯酸在纳米TiO2表面吸附行为的研究

讨论了聚丙烯酸在纳米TiO₂水悬浮体系中的吸附行为.红外光谱分析和吸附实验结果表明,纳米TiO₂通过氢键吸附PAA.PAA吸附量随着浓度的升高而增大直至饱和吸附量,且分子量越大,饱和吸附量越大.pH值增大,则饱和吸附量减小.在相同条件下,表面吸附层的厚度随PAA分子量、浓度和pH值增大而增大.这是由PAA在颗粒表面构型的变化所致.吸附PAA后的纳米TiO₂的表面电荷密度和ζ电位发生变化,pHiep值向低值方向移动.表面吸附自由能的计算结果说明,PAA在纳米TiO₂表面的吸附是自发过程.     

活性炭的zeta电位对各种染料吸附的影响3．活性炭对阴离子染料洋红的吸附

测定了在不同pH下活性炭吸附阴离子染料洋红的变化规律,发现活性炭表面的电位(ζ对洋红吸附量的影响起着重要作用.当溶液pH小于活性炭的零电位pH(pHZPC=6.2)时,活性炭表面带正电,它对洋红阴离子具有静电引力,而当pH增大时活性炭的ζ电位下降,静电引力减弱,使得吸附量下降;另一方面由于洋红变色(pH3.5橙色,～pH6.8玫瑰红)后,洋红的溶解度增大,所以导致吸附量很快下降并趋于零.通过活性炭对洋红在不同pH下的吸附动力学和吸附热力学参数的估算,进一步揭示了活性炭在不同pH下对洋红的吸附机理.     

木质素磺酸盐在烯酰吗啉颗粒表面的吸附特性

考察了常用分散剂木质素磺酸钠(Sodium Lignosulfonate, SLS)在烯酰吗啉(Dimethomorph, DMM)上的吸附性能, 并测试了吸附SLS后DMM颗粒表面Zeta电位和接触角的变化, 从理论上探讨了分散剂的吸附对农药颗粒表面物化性能的影响, 指导农药分散剂的开发. 结果显示, 浓度为0~10 g/L时, SLS在DMM表面呈现双层吸附; 低浓度(0~1.0 g/L)时, 吸附等温线符合Langmuir方程. SLS在DMM表面上的吸附属于自发、 放热吸附过程, 吸附力主要包括疏水作用、 范德华力和氢键作用力. SLS在DMM表面吸附后提高了其Zeta电位, 且SLS磺化度越高其提高作用越明显. 随着SLS溶液浓度增大, DMM在SLS溶液中的接触角先减小后增大, 到70º~80º后趋于稳定.     

不同分子质量木质素磺酸钠对煤粉的分散作用研究

应用超滤分级方法,将木质素磺酸钠分成不同分子量范围的级分。傅立叶红外光谱（FTIR）分析结果表明,分子量为5 000～10 000的木质素磺酸钠分子中亲水基团如羟基、酚羟基、磺酸根质量分数最大,随着分子量的增加,亲水基团质量分数降低。实验结果发现分子量为10 000～50 000的木质素磺酸钠级分在煤粒表面的吸附等温线近似为L型,吸附量较大,并且使煤粒的表面动电电位（ζ电位）达到-52 mV,在各个级分中对盘江煤具有最好的分散降黏作用。进一步得出结论,分散剂的分散降黏作用与其在煤粒表面的吸附量和ζ电位的高低密切相关。     

分散剂表面吸附特性和相关电化学性质对煤浆分散体系流变特性的影响

采用１７种不同变质程度的中国煤，详细研究了一种阴离子型分散剂在煤表面的吸附特性及其相关的表面电化学性质对煤成浆性及浆体流变特性的影响。结果表明，煤成浆性及浆体流变性并不单独取决于煤对分散剂的吸附量和煤表面动电位的大小。反映煤成浆性的浆体最高煤浆浓度取决于分散剂在煤表面的Ｌａｎｇｍｕｉｒ饱和吸附量Γｓ和相应动电位ξｓ的乘积Γｓ×ξｓ，而浆体流变指数则依赖于两者比值的大小Γｓ／ξｓ。表明水煤浆分散体系中煤颗粒的分散一方面是靠静电分散作用来实现，另一方面，分散剂在煤表面的吸附所产生的非静电分散作用也起了重要作用。同时，分散剂的表面吸附使煤表面产生的吸附荷电效应不能过高，否则，会对流体流变性不利。     

Adsorption of modified dextrins on talc: effect of surface coverage and hydration water on hydrophobicity reduction

The adsorption of three modified dextrins on the basal plane of talc has been studied using in situ tapping mode atomic force microscopy (TMAFM). The images have been used to determine the layer thickness and coverage of the adsorbed polymers. Adsorption isotherms of the polymers on talc particles were also determined using the depletion technique. Values of the adsorbed amount at equilibrium were compared with the volume of adsorbed material as determined using in situ TMAFM, revealing the presence of significant amounts of hydration water in the adsorbed layer structure. This deduction was confirmed by comparing in and ex situ TMAFM images of the adsorbed dextrins. The effect of layer thickness, coverage, and hydration water content on the contact angle of talc particles treated with polymer was investigated using the Washburn method and the equilibrium capillary pressure (ECP) method. Distinct correlations were observed between adsorbed layer properties and the measured contact angles, with the ECP measurements especially highlighting the effect of the adsorbed polymer layer hydration water. The implications for the performance of the modified dextrins in flotation are discussed.     

双梳型共聚物在莠去津颗粒表面吸附的X射线光电子能谱分析

采用X射线光电子能谱(XPS)研究了双梳型共聚物吸附于莠去津颗粒样品表面的电子状态,计算了吸附厚度.结果表明:吸附后,莠去津颗粒界面的N 1s和Cl 2p谱峰强度明显减弱,Cl 2s几乎消失,而C 1s和O1s谱峰强度则明显增强,这主要是双梳型共聚物中C和O的贡献,且吸附后能在莠去津颗粒界面形成良好的吸附保护膜,其厚度...     

Numerical study of the equilibrium properties of suspended particles surrounded by a permeable membrane with adsorbed charges

The network simulation method is used to calculate the electrostatic potential distribution for suspended spherical particles made of a charged core surrounded by a permeable membrane with adsorbed charges. The structure of the equilibrium diffuse double layers on both sides of the membrane-electrolyte solution interface is analyzed considering an anion adsorption process described by a Langmuir-type isotherm. It is shown that the thickness of the double layer in the membrane strongly depends on the adsorption constant, while it is almost independent of this constant in the electrolyte solution. The evolution of the electric potential on the core as a function of the electrolyte concentration is also analyzed.     

Stabilization of gamma alumina slurry for chemical-mechanical polishing of copper

Stabilization of gamma-alumina suspension for chemical-mechanical polishing (CMP) of copper was investigated. Citric acid and poly(acrylic acid) (PAA) (M(w)=5000) were used as dispersant. The stability of suspension was evaluated from the changes in viscosity, particle size and zeta potential. It appears that metastable gamma-alumina mainly due to its high specific surface area and to the presence of aluminol groups on its surface is progressively transformed to bayerite (beta-Al(OH)(3)) by hydration procedure. Citric acid molecules were adsorbed onto gamma-alumina surface effectively and exhibited the excellent hydration inhibition effect. Although citrate-alumina surface complexes give barrier to the flocculation, the repulsion potential is based mainly on the electrostatic repulsion, thereby steric hindrance caused by the adsorption of these small molecules is very weak. The electrosteric repulsion, which provides more effective dispersion stability than electrostatic repulsion force, can be expected by using polyelectrolyte such as PAA; however, adsorbed layers of PAA onto solid/liquid interface are loosely formed. Therefore, a large amount of PAA was required to inhibit the surface hydration of gamma-alumina suspension, thereby the excess addition of PAA decreased the electrosteric repulsion and re-bridging of the dispersant between particles caused an increase in suspension viscosity. Therefore, synergistic effect can be expected in mixed dispersant system of citric acid and PAA, since small citric acid molecules are adsorbed faster than PAA, inhibiting the progress of surface hydration, and then adsorbed PAA layers exhibit the effective electrosteric repulsion interaction between particles with a small amount compared with PAA alone. It was revealed that the gamma-alumina slurry dispersed by mixed dispersant exhibited the improved removal rate of Cu layer by CMP polishing test.     

Flow of solutions in thin capillaries coated with an adsorbed polyelectrolyte lyer

The flow of KCl solutions through thin quartz capillaries coated with an adsorbed layer of a cationic polyelectrolyte (CPE), poly(dimethyldiallylammonium chloride) (molecular mass M = 500000), is studied. It is found that the adsorption layer is soft and its thickness depends on shear stress generated by the liquid flow through the capillary. The hydrodynamic thickness of the CPE adsorption layer is 80–90 nm at low flow rates of a solution, and it decreases to values comparable with the experimental error at high flow rates. The dried adsorption layer appears to be hydrophobic (the advancing contact angle is about 80°); in these capillaries, the flow rate of a KCl solution is increased that can be interpreted as a solution slip on the surface of CPE adsorption layer. The long-term contact of the dried CPE adsorption layer with KCl solution, probably, results in the swelling of the adsorption layer, which is accompanied by a decrease in the contact angle and ζ potential of the adsorption layer surface as calculated from the streaming potential of the same solution.     

Effect of alkylpyridinium chlorides on aggregation stability of aqueous dispersions of detonation nanodiamonds

Adsorption of decyl-, dodecyl-, and hexadecylpyridinium chlorides (DePC, DoPC, and CPC, respectively) from aqueous solutions on the surface of detonation nanodiamonds (NDs) and its effect on the aggregation stability of ND hydrosols are studied. Hydrophobic interactions, which are enhanced with the length of hydrocarbon chains in surfactant molecules, are found to play the main role in surfactant adsorption on the ND surface. DePC is almost not adsorbed on NDs, and its addition has no effect on both the size and ζ potential of nanoparticles. Adsorption of DoPC decreases the ζ potential of ND particles, thus causing their coagulation. Superequivalent adsorption of CPC results in sign reversal of the ζ potential of ND particles, thereby leading to alternation of the zones of aggregation stability and coagulation of the hydrosols with a rise in the concentration of this surfactant.