高分子共混体系界面张力的研究

<正> 在高分子多相体系中,相间界面张力(γ_(12))是微区的重要控制因素,无论是Donatelli,Sperling等提出的IPN体系微区尺寸关系式,还是Tokita提出的共混体系中分散相粒径表达式,都含有界面张力因子。 然而,由于高分子体系中界面张力测定的诸多实际困难,当前在国内外非常多的研究工作中,广泛地采用了一些替代的办法,应用较多的有以表面张力差来代替界面张力的Antonow原则延伸及一些近似的计算方法,如Wu及Girifalco和Good提出的由表     

CMC系列高分子表面活性剂与原油超低界面张力形成机理的研究

采用动态激光光散射及环境扫描电镜研究了羧甲基纤维素系列高分子表面活性剂与大庆原油形成超低界面张力的机理.结果表明,CMC系列高分子表面活性剂具有与低分子量表面活性剂相比拟的表/界面活性,其水溶液的表面张力可达2835mN/m,界面张力达到10^-110mN/m.碱的加入可显著降低高分子表面活性剂与原油的界面张力,在适当条件下界面张力达到超低值(10^-3mN/m),可望作为三次采油的驱油剂.等效烷烃模型研究表明,用碱与原油酸性组分的作用来解释碱能使界面张力下降至超低值的传统观点是不完善的,加入碱能使高分子表面活性剂胶束解缔,胶束数量增多,胶束粒径减小,单分子自由链增加,有利于高分子表面活性剂向界面迁移和排布,这是高分子表面活性剂和碱复配体系与原油界面张力下降至超低值的主要原因.     

质子平衡方程各组分浓度动态图与碳酸氢钠溶液pH计算

NaHCO₃水溶液的质子平衡方程为：[H₂CO₃]+[H⁺]=[OH^-]+[CO■]。随溶液浓度c的变化,H₂CO₃,H⁺,OH^-和CO■的相对含量也会发生变化。提出并绘制了质子平衡方程中各组分浓度随溶液浓度c变化的动态图。从动态图上,可以直观地观察到哪些组分是主要组分,哪些组分是次要组分,哪些组分相对含量可以忽略不计,从而得到不同浓度区间溶液的不同pH近似式。对动态图的研究,不仅可以发现新的pH近似式,还可以帮助正确解读pH近似式的物理意义。值得强调的是,动态图对溶液中存在的各类质子转移平衡也能提供全新的认识。较浓溶液中,质子转移平衡■占据支配地位。9.1×10^-6 mol·L^-1稀溶液中,反应■^-占据支配地位。     

表面活性剂亲水-亲油能力对动态界面张力的影响

当两个不互溶的液相接触时 ,如果其中一相或两相含有表面活性物质 ,就可能产生动态界面张力 .两相间的界面张力随时间连续变化 ,直到平衡为止 .在到达平衡的过程中 ,经常通过一个最低值 .酸 性油 /碱水体系也会出现类似现象 .England和 Berg[1]把动态界面张力解释为表面活性物质在界面上累积的结果 ,并观察到 1,5-戊二醇由白油向水 中传质时存在明显的吸附-脱附位垒 .Rubin和 Radke[2]首次给出了解释酸性原油与碱水溶液接触时产生动态界面张力的物理模型 ,他们提出在油水界面上存在一个表面活性物质的脱附位垒 ,原油中的酸性物质与氢氧化…     

新型三硅氧烷表面活性剂的合成与界面性能

低聚乙二醇单甲醚和环氧氯丙烷在相转移催化剂(P.T.C)存在下合成出低聚乙二醇甲醚缩水甘油醚, 然后与氨丙基三硅氧烷进行开环反应, 合成出了新型的三硅氧烷表面活性剂Me₃SiOSiMeROSiMe₃ [R＝(CH₂)₃N(CH₂CH(OH)CH₂- (OCH₂CH₂)_xOCH₃)₂, x＝1, 2]. 通过¹H NMR确证了这些目标产物的结构, 并且通过测定其水溶液的平衡表面张力研究了其表面活性. 在浓度约为10^－4 mol•L^－1时可以将水的表面张力降低至约21～22 mN•m^－1.     

十六烷基甲苯磺酸钠的界面性能研究

用自制的3种十六烷基甲苯磺酸钠,研究了其正构烷烃/水体系的界面性能。分别考察了磺酸盐支化程度及浓度等内部因素以及外加助剂脂肪醇类型和无机盐浓度等外界因素对磺酸盐最小烷烃碳数n_min以及界面张力值的影响。结果表明,磺酸盐支化程度增加,其n_min变大,最低界面张力值变小;而随着磺酸盐浓度的增加,界面张力值先下降后上升;随着助剂脂肪醇碳链长度的增加,其n_min逐渐变大;无机盐的影响则表现为随着盐浓度的增加界面张力值先下降后上升,超低界面张力值出现在一个适宜的盐浓度范围内。     

系列烷基苯磺酸盐对烷烃的动态界面张力研究

从表面活性剂分子量、表面活性剂浓度、电解质浓度、烷烃碳数等方面考察了系列烷基苯磺酸盐异构体纯化合物的油水动态界面张力行为.研究表明,表面活性剂分子量增大和电解质浓度增加使界面张力动态变化减慢,达到平衡所需时间延长;表面活性剂浓度增加和烷烃碳数增加使界面张力动态变化加快,达到平衡所需时间减少.     

液滴在不互溶液体表面上的相对界面自由能曲面及Neumann三角形的导出

根据系统的界面Helmholtz自由能自发地趋于最低的热力学原理,以浮在不互溶液体(2)表面上透镜状液滴(3)在气(1)、液₂、液₃三相交界处,气-液₃、液₂-液₃界面各自和气-液₂界面通过液滴内部的夹角θ₁、θ₂为变量(0°≤θ₁≤180°,0°≤θ₂≤180°),证明出3个界面张力γ₁₂、γ₁₃、γ₂₃各种可能组合情况下液体₃稳定时的θ₁、θ₂值与它们之间的关系,导出Neumann三角形;并按照计算数据绘出几种类型相对于气相中圆球形液滴的界面自由能曲面图。     

诱导期测定法对碳酸锂成核动力学的研究

在288.15～323.15 K温度范围内,采用诱导期测定法研究了碳酸锂(Li₂CO₃)在有无添加NaCl的Li Cl-Na₂CO₃过饱和溶液中的成核动力学.通过OLI电解质与水化学物性分析软件内嵌的全组分模型严格计算Li₂CO₃在溶液中的过饱和度,研究了温度、过饱和度和Na Cl的添加量对Li₂CO₃成核诱导期的影响,并结合经典初级成核理论计算了活化能、固-液界面张力和接触角等成核动力学参数.结果显示,在相同的过饱和度下,Na Cl的添加使得Li₂CO₃的成核诱导期增长;添加Na Cl后Li₂CO₃成核反应的活化能从63.69 k J/mol(溶液中Cl^?的超额含量Y=0)增加到72.85 k J/mol(溶液中Cl^?的超额含量Y=0.5),表明Na Cl的添加抑制了Li_...     

中性载体ETH1117推动H+通过水/硝基苯界面传递的电化学研究

用循环伏安法研究中性载体ETH1117推动H⁺通过水/硝基苯界面的转移。通过络合使H⁺穿过水/硝基苯界面转移,是受扩散控制的可逆过程,ETH1117与H⁺在硝基苯相的配合比为1:1,配合物的稳定常数β₀为2.9×10⁷,扩散系数D为4.2×10^-6cm²/s。     

Sorbent Concentration Effect on Adsorption of Methyl Orange on Chitosan Beads in Aqueous Solutions

The adsorption of methyl orange（MO） on chitosan（CS） beads in aqueous solutions was investigated by a batch equilibration technique. Special emphasis was focused on the effect of sorbent concentration（cs） on the adsorp- tion equilibration of MO on CS beads. An obvious Cs-effect was observed in the adsorption equilibration, i.e., the ad- sorption amount（F） was declined with Cs increase. The classical Langmuir model adequately described the adsorption isotherm for each given cs. However, it could not be used to predict the cs-effect observed. The applicability of the Langmuir-SCA isotherm, a surface component activity（SCA） model equation, to fit the cs-effect data was examined. In the SCA model, the activity coefficient of sorbent surface sites, fsH2O, was assumed to be a function of cs due to the deviation of a real adsorption system from an ideal one, arisen from sorbent particle-particle interactions in real systems. The results show that the Langmuir-SCA isotherm could accurately describe the c：effect observed under the studied conditions. Furthermore, the effects of temperature（t）, pH, and electrolyte（NaNO3） concentration（ CNaNO3 ） on fsH2O were examined. The results show that fsH2O clearly decreased with increasing t（20-35℃） and pH（5-8）, but no obvious change in fsH2O was observed as CNaNO3 varied in a range 0.001-0.010 mol/L. These results give a better understanding of the cs-effect.     

氧化反应对胜利褐煤水蒸气气化反应的促进作用Ⅰ:宏观反应特性研究

在φ80×3 000mm耐高温不锈钢管气流床反应器中,以150-180μm胜利褐煤为气化原料,考察了800和900℃时添加氧气前后褐煤转化率的变化,研究了氧化反应对水蒸气气化反应影响的宏观特征。结果表明,添加氧气后褐煤转化率明显大于O_2和H_2O气氛下褐煤转化率之和,即向水蒸气气氛添加氧气后褐煤转化率的增幅大于氧气氧化作用导致的褐煤转化率的增幅,随着H_2O含量增大以及温度的升高此现象愈加明显。该协同作用主要是氧化反应对水蒸气气化反应的促进作用造成的。利用φ40×200 mm石英圆筒流化床反应器进行了类似的实验,也发现了该协同作用。同时,借鉴收缩核模型并结合气流床气化实验条件推导了水蒸气气化宏观动力学方程,得到的速率方程(Z-(1-x))~(1/3)=(tβk_(H_2O)/Rρ_C)φ_(H_2O)=K_(H_2Oφ_(H_2O))与实验值吻合较好,添加氧气后水蒸气气化反应速率和水蒸气气化反应表观速率常数K_(H_2O)明显增大,这是氧气对水蒸气气化反应促进作用的动力学特征。     

Adsorption and desorption kinetics of CmE8 on impulsively expanded or compressed air–water interfaces

The adsorption kinetics of C_mE₈ (m=10, 12, and 14) at an air–water interface are investigated. A pendant bubble is formed in aqueous surfactant solution and allowed to attain equilibrium. The bubble is then impulsively expanded or compressed with some change of area large enough to appreciably deplete or enrich the surface concentration and change the surface tension. The surfactant is then allowed to re-equilibrate. The surface tension evolution during this process is measured using video images of the pendant drop. The surface tension evolution is compared to mass transfer arguments. First, the re-equilibration of interfaces laden with C₁₄E₈ are studied. For compressed interfaces, surfactant must desorb to restore equilibrium. The surface tension rises more slowly than predicted by a diffusion-controlled evolution, implying that the re-equilibration is mixed diffusive-kinetic controlled. By analyzing the surface tension evolution in terms of a mixed kinetic-diffusive model, values for the kinetic constants for adsorption and desorption are found. These results are compared to those obtained previously for C_mE₈ (m=10 and 12). For all of these molecules, the adsorption rate constant is similar (β₁=5.6±1.0×10⁻⁶ cm³ (mol s)⁻¹). However, the desorption rate constant (₁) varies strongly. Increasing m by 2 lowers the desorption rate constant ₁ by nearly a factor of 15. This is consistent with an increased resistance to re-immersion into water with the length of a hydrocarbon chain.     

双子表面活性剂Dynol-604溶液的动态表面张力研究

通过测定双子表面活性剂Dynol-604的动态表面张力(DST),研究了温度和浓度等对其DST的影响,详细表征了DST随时间的变化过程,计算了动态表面张力的各种参数(t_i,t^*,t_m,R_1/2).结果表明,其表面张力降低迅速,γ_m值也很低.探讨了上述参数的物理意义和变化规律.     

Investigation Static/Dynamic Surface and Interfacial Tension of Some Synthesized Polymeric Surfactants to Enhance the Egyptian Jet Fuel A1 Atomization

In the present work some exthoxylated polyalkylphenol surfactants have different alkyl chains (nonyl and dodecyl) were synthesized. The static surface tension for these surfactants in water and jet fuel A1 was measured and the critical micelle concentration (CMC) for each surfactant was determined. The data show the general trend of decreasing the CMC against the molecular weight of the synthesized polymeric surfactants. The HLB of these surfactants was also calculated. The dynamic surface tension for the synthesized surfactants was measured at CMC. The dynamic interfacial tension for these surfactants with jet fuel A1 at CMC was also measured using the spinning drop technique. The results showed that the effect of the synthesized surfactants on deceasing the time of droplet maturation was significant remarked. The decrease of this time leads to enhance of jet fuel atomization.     

球型胶体颗粒的表面电位和表面电荷密度的关系

胶体颗粒的表面电荷密度和表面电位之间的关系是颗粒表面的基本性质之一．要确定这个关系,需要解Poisson-Boltzmann(PB)方程,求出颗粒外的电位分布．然而对于球形颗粒,PB方程却没有解析解．Loeb等,求出了数值解,近似解析表达式虽然很多,也比较复杂,     

O2/CO2气氛下污泥/煤混燃中半挥发性重金属的释放特性

在固定床焚烧实验装置上,采用正交实验法研究了焚烧温度(t_c)、污泥掺混比(X_s)、O_2体积分数(φ_(O2))、初始含水率(φ_(H2O))、焚烧时间(τ)和含氯量(φ_(Cl))六个因素对O_2/CO_2气氛下污泥/煤混燃中半挥发性重金属(Zn、Pb、Cd、Cu、Ni和Cr)释放特性的影响。结果表明,六种因素对重金属释放率影响程度排序为t_cX_sφ_(H2O)φ_(O2)≈τφ_(Cl)。相同焚烧工况下,Zn释放率最大,Pb和Cd次之,Cu、Ni和Cr较小。提高温度会促进重金属释放,且高温(1000-1100℃)对重金属释放的影响显著强于低温(700-900℃)。随着温度由700℃升高至1100℃,Zn和Pb释放率分别由36.1%和12.2%上升至70.9%和63.5%,Cd在900℃下达到40.0%的最大释放率,而Cu、Ni和Cr释放率大都维持在20.0%以下,温度对重金属释放率影响程度排序为PbZnCdCuCrNi。重金属释放率随着污泥掺混比增加逐渐下降,却随着初始含水率增加呈现波浪式变化趋势,且在30%O_2体积分数下重金属释放率取得最小值。焚烧时间和含氯量对Pb释放的影响程度显著强于其他五种重金属。O_2/CO_2气氛下污泥/煤混燃的最佳工况为:焚烧温度为900-1000℃、污泥掺混比为25%左右、O_2体积分数为30%、初始含水率小于10%,并尽可能的缩短焚烧时间。     

Study on the Mechanism of Asphaltenes Reducing Oil-Water Interfacial Tension

As high polar components of crude oil, asphaltenes play a significant role in reducing oil-water interfacial tension(IFT). In this paper, the effects of asphaltenes on reducing IFT in the presence of surfactant were compared, and the mechanism of asphaltenes reducing the IFT was studied by the dynamic interfacial tension(DIFT) equation. Whether asphaltenes were added to the oil or 2,5-dimethyl-4-(4-dodecyl) benzene sodium sulfonate(p-S14-4) was added to the water phase, either of all results in the IFT reducing and the IFT is related to the coverage and the mass of asphaltenes adsorption at the interface. In the presence of asphaltenes, the adsorption of the active substances to the interface is not entirely dependent on diffusion, and the process can be divided into three regions. Region I: the IFT rapidly reducing, this process is controlled by diffusion of surfactant; Region II: the IFT reducing slowly, resulted from the lower diffusion rate that is limited due to the aggregates formed by the interaction of asphaltene-asphaltene; Region III: the interaction of asphaltene-asphaltene is broken by the interaction of surfactant-asphaltene. The asphaltene aggregates are reduced and adsorbed rapidly at the interface. Furthermore, the results reveal that the asphaltenes concentration affects the coverage rate and adsorption at the interface.     

蓖麻油酸甲酯乙氧基化物水溶液的动态表面张力

用最大气泡压力法分别测定了不同环氧乙烷(EO)加合数(10、12、14、16、20)的蓖麻油酸甲酯乙氧基化物(ECAME)水溶液的动态表面张力(DST)。考察了浓度、温度和无机电解质对DST的影响,探讨了不同浓度时DST参数(动态表面张力特性参数n,平衡时间t^*,曲线最大斜率R_1/2)的变化规律。结果表明,随着EO数由10增加到20,DST不断增大;随着浓度由0.5×10^-5 mol/L增加到10×10^-5 mol/L,n由3.02减小到1.05,t^*值由14.45减小到2.29,R_1/2由0.43增大到6.44,则动态表面活性增大,DST降低;随着温度由25 ℃升高至45 ℃,DST降低;吸附初期DST曲线随无机电解质浓度的增大而升高,吸附后期DST曲线随无机电解质浓度的增大而降低。和常规的脂肪酸甲酯乙氧基化物(FMEE)相比,ECAME的动态表面活性更加优异,这为开拓ECAME的应用指明了新的方向。     

1-甲氧基乙基-3-甲基咪唑甘氨酸离子液体的物理化学性质的研究

由于氨基酸基的独特性质,我们以甘氨酸作为阴离子,醚基咪唑基团作为阳离子合成了一种新型离子液体1-甲氧乙基-3-甲基咪唑甘氨酸[MOEMIM][Gly],并经过核磁共振氢谱、核磁共振碳谱和差示扫描量热进行表征。由于离子液体和水之间形成氢键导致传统的方法不能去除水的影响,所以在实验测定中,选用标准加入法在温度范围为298.15–338.15 K,每隔5 K测定离子液体[MOEMIM][Gly]的密度和表面张力。利用密度数据,计算得到离子液体[MOEMIM][Gly]的摩尔体积,并且摩尔体积随着温度的升高而增加,同时得到了热膨胀系数。根据离子液体[MOEMIM][Gly]的摩尔表面Gibbs自由能,改进了传统的Eötvös经验方程,使得方程具有更明确的物理意义,即截距C₀代表摩尔表面焓,它是一个与温度无关的常数,斜率则为摩尔表面熵,这表明改进的Eötvös方程不仅是一个经验方程,而且还是严格的热力学方程。另外,结合摩尔表面Gibbs自由能和改进的Eötvös方程,估算了离子液体的[MOEMIM][Gly]的表面张力,并与实验值进行比较,发现两者很好的一致。