共查询到19条相似文献,搜索用时 62 毫秒
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气/液界面上十六烷基三甲基溴化铵水溶液的动态表面性质 总被引:4,自引:0,他引:4
用最大泡压法测定了不同温度下浓度低于cmc时十六烷基三甲基溴化铵水溶液的动态表面张力.发现当浓度低于0.10
mol·m-3时动态吸附量ΓT遵s从由Henry吸附等温式导出的动态表面状态方程.在浓度位于0.10至0.80mol·m-3的较大范围内,Tt遵从从Langmuir等温式导出的动态表面状态方程.在吸附的后期十六烷基三甲基溴化铵分子在溶液表面上的吸附遵从混合动力学控制机理.从表观扩散系数计算出吸附为混合动力学控制机理时吸附能垒为6.7~7.1
kJ· 相似文献
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钙矾石3CaO·Al2O3·3CaSO4·32H2O是水泥熟料水化的重要产物.它易被空气中的CO2 分解,常温下的分解反应为3CaO·Al2O3·3CaSO4·32H2O 3CO2 →3CaCO3 Al2O3·xH2O 3(CaSO4·2H2O) (26 -x)H2O分解机理[1 ,2]是:H2O先吸附在钙矾石表面的活性中心上,吸附态水再吸收CO2 成为H2CO3 ,然后碳酸与钙矾石反应,实现碳化(即分解).其分解速率[3]为v=kpco2 pH2o(1)可见水的吸附是钙矾石碳化分解的关键步骤,因此探讨… 相似文献
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用最大泡压法考察季铵盐Gemini表面活性剂C12-2-Ex-C12?2Br (x=1, 2, 3)在气/液表面吸附动力学行为, 研究表明增加表面活性剂体相浓度和温度将加快分子扩散速度, 因此提高了表面吸附的动力学效果. 增加联接链长度x减小了分子预聚集倾向, 溶液中的单分子浓度增加, 有利于初始扩散, 使γt降低. 接近饱和吸附时, 由于x较大的单元分子在表面层占据的截面积也较大, 降低了表面层甲基端基的覆盖度, 相对升高了介平衡表面张力. 与对应的同头基同碳原子数的十二烷基三甲基溴化铵(C12TABr)比较, C12-2-E1-C12?2Br分子更倾向于吸附在表面层上. 相似文献
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最大泡压法研究C12-2-Ex-C12•2Br在气/液表面的吸附动力学 总被引:3,自引:0,他引:3
用最大泡压法考察季铵盐Gemini表面活性剂C12-2-Ex-C12?2Br (x=1, 2, 3)在气/液表面吸附动力学行为, 研究表明增加表面活性剂体相浓度和温度将加快分子扩散速度, 因此提高了表面吸附的动力学效果. 增加联接链长度x减小了分子预聚集倾向, 溶液中的单分子浓度增加, 有利于初始扩散, 使γt降低. 接近饱和吸附时, 由于x较大的单元分子在表面层占据的截面积也较大, 降低了表面层甲基端基的覆盖度, 相对升高了介平衡表面张力. 与对应的同头基同碳原子数的十二烷基三甲基溴化铵(C12TABr)比较, C12-2-E1-C12?2Br分子更倾向于吸附在表面层上. 相似文献
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溶液表面吸附实验数据的计算机非线性拟合法处理 总被引:1,自引:0,他引:1
通过Gibbs公式与Langmuir等温式的结合 ,对溶液表面吸附实验进行数据处理 ,得到两组分稀溶液表面张力σ与溶液浓度c关系式。用计算机进行非线性函数拟合代替传统的作图、作切线、再直线拟合的方法。该方法具有简单快捷、拟合参数能直接反映实验数据质量的特点 相似文献
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用振荡射流法分别测定了不同温度下全氟辛酸、十二烷基硫酸钠、二聚氯乙烯正辛醇醚溶液(浓度低于CMC)的动表面张力,讨论了它们的表面吸附动力学,研究结果表明都是扩散控制。 相似文献
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The surface tension of a solid, unlike that of a liquid, cannot be measured directly. After a discussion of the most important methods used so far, all of which are subject to uncertainty the determination of the surface tension of solids from the wetting equilibrium is described. 相似文献
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In the solution adsorption experiment, different adsorption mode has been observed for aqueous ethanol and aqueous n-butanol, respectively. However, it is difficult to make an adjustment by the profiles of σ-c relationship. Choosing the experimental conditions improperly will give wrong results. Since there is no consistency between the Gibbs adsorption isotherm and Langmuir adsorption isotherm, the experimental data should not be fitted by using any algebraic equations or physical models. The data fitting for this experiment should be carried out according to the following steps:fitting the σ-lnc curve manually, making it monotonic and smooth; retrieving more data from this fitting curve, and re-plotting the σ-lnc curve; calculating the first derivatives at these data points (i.e., (∂σ/∂lnc)T); calculating surface adsorptions by Gibbs adsorption isotherm, Γ=-(∂σ/∂lnc)T/RT. As for the calculation of the cross-section area for the solute molecule, the effect of concentration of bulk solution (i.e., c) on the surface molecular density should be taken into account. 相似文献
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《Journal of Dispersion Science and Technology》2013,34(6):745-751
Dodecyl polyoxyethylene(4) polyoxypropylene(5) ether (LS45) is an outstanding microemulsifier in supercritical CO2. The dynamic surface tension (DST) of this nonionic surfactant was investigated by using the maximum bubble pressure instrument. The effects of concentration and temperature on DST parameters (n, ti, t*, tm, and R1/2) and its adsorption mechanism were discussed by Rosen's empirical equation and the asymptotic Ward and Tordai equation for the LS45 solution system. Finally, the parameters at 1 s related to Draves's wetting performance, pC20(1s), C1s (i)*, and C1s*, analyzed. The results showed that were with increase of bulk concentration and temperature, dynamic surface activity increased. Parameters at 1 s indicated that LS45 is of high surface activity and a very good wetting agent. One‐second related parameters, C1s (i)* and C1s*, are valuable in the treatment of practical applications of surfactants. Optimum wetting can be expected at the concentration of 4.8×10?4 mol/dm3 for LS45 solution. 相似文献
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WANGFeng-kun WUJiang-tao LIUZhi-gang 《高等学校化学研究》2005,21(2):205-208
A generalized corresponding-state model based on two reference fluids was developed for the prediction of surface tensions for non-polar and weakly polar pure fluids and their binary mixtures. Four parameters,po, Tc, Vc and ω, were used in this model, and the acentric factor ω was used as a scaling parameter. This model has been tested for 69 pure substances and 20 binary mixtures; the average absolute deviations are 0. 28 and 0. 20 mN/m, respectively. The results indicate that the predictions by means of this model were in good agreement with experimental data. In addition, the calculated deviation would increase with the excess surface tension rising, and if the excess surface tension is less than 3 mN/m, the prediction will be good and credible. 相似文献