Azizian S, Shibata K, Matsuda T, Takiue T, Matsubara H, Aratono M
Department of Chemistry, Faculty of Sciences, Kyushu University, Hakozaki 6-10-1, Higashiku, Fukuoka 812-8581, Japan.
J Phys Chem B. 2006 Aug 31;110(34):17034-42. doi: 10.1021/jp063301p.
The surface conformational states of the Gibbs monolayer of ethylene glycol mono-n-dodecyl ether (C(12)E(1)) at the air/water interface was studied using dynamic surface tension, external reflection-absorption FT-IR spectroscopy (ERA FT-IR), and two-dimensional infrared (2D IR) correlation methods at constant temperature. The dynamic surface tensions were measured at different bulk concentrations of C(12)E(1), and it was observed that a constant surface tension region appears at approximately 38.5 mN m(-1) in a dynamic surface tension profile at concentrations higher than 11 micromol kg(-1). This constant surface tension region corresponds to the surface phase transition from liquid expanded (LE) to liquid condensed (LC). Two sets of ERA FT-IR spectra were collected, one at different bulk concentrations but after equilibrium time (equilibrium measurements) and another at constant bulk concentration (m = 16 micromol kg(-1)) but at different times (dynamic measurements). The first set of these measurements show that the peak area increases in the range of 11 < m < or = 16 micromol kg(-1), which means the increase in the number of surfactant molecules at the air/water interface. Also, the wavenumber of antisymmetric CH(2) stretching decreases gradually from approximately 2923 cm(-1) (for 10 and 11 micromol kg(-1)) to approximately 2918 cm(-1) (for m > or = 16 micromol kg(-1)) with increasing concentration. The wavenumbers of 2923 and 2918 cm(-1) were assigned to LE and LC phases, respectively, and the decrease of wavenumber in the concentration range of 11 < m < or = 16 micromol kg(-1) were correlated to the surface phase transition (LE --> LC), or in other words, in the mentioned concentration range, two phases coexist. The dynamic ERA FT-IR measurements at 16 micromol kg(-1) also confirm the surface phase transition from LE to LC. The 2D IR correlation method was applied to the both equilibrium and dynamic IR spectra of the C(12)E(1) monolayer. The synchronous correlation maps show two strong autopeaks at approximately 2922 and approximately 2851 cm(-1) and also show a strong correlation (cross-peaks) between antisymmetric CH(2) stretching (nu(a)) and symmetric CH(2) stretching (nu(s)). The asynchronous correlation maps show that both observed bands of nu(a) and nu(s) in one-dimensional IR split into two components with the characteristic of overlapped bands, which reveals the coexistence of two phases (LE and LC) at the interface at 11 < m < or = 16 micromol kg(-1). The synchronous and asynchronous maps that were obtained from dynamic IR spectra closely resembled the equilibrium map.
在恒温条件下,采用动态表面张力、外反射吸收傅里叶变换红外光谱(ERA FT - IR)和二维红外(2D IR)相关方法,研究了乙二醇单正十二烷基醚(C(12)E(1))在空气/水界面的吉布斯单层膜的表面构象状态。在不同的C(12)E(1)本体浓度下测量动态表面张力,发现在浓度高于11 μmol kg(-1)时,动态表面张力曲线中约38.5 mN m(-1)处出现一个恒定表面张力区域。这个恒定表面张力区域对应于从液体扩张(LE)到液体凝聚(LC)的表面相变。收集了两组ERA FT - IR光谱,一组是在不同本体浓度但达到平衡时间后(平衡测量),另一组是在恒定本体浓度(m = 16 μmol kg(-1))但不同时间(动态测量)。第一组测量结果表明,在11 < m ≤ 16 μmol kg(-1)范围内,峰面积增加,这意味着空气/水界面处表面活性剂分子数量增加。此外,随着浓度增加,反对称CH(2)伸缩振动的波数从约2923 cm(-1)(对于10和11 μmol kg(-1))逐渐降低到约2918 cm(-1)(对于m ≥ 16 μmol kg(-1))。2923和2918 cm(-1)的波数分别对应于LE相和LC相,在11 < m ≤ 16 μmol kg(-1)浓度范围内波数的降低与表面相变(LE→LC)相关,或者换句话说,在上述浓度范围内,两相共存。在16 μmol kg(-1)下的动态ERA FT - IR测量也证实了从LE到LC的表面相变。将2D IR相关方法应用于C(12)E(1)单层膜的平衡和动态红外光谱。同步相关图谱在约2922和约2851 cm(-1)处显示出两个强自峰,并且在反对称CH(2)伸缩振动(ν(a))和对称CH(2)伸缩振动(ν(s))之间也显示出强相关性(交叉峰)。异步相关图谱表明,在一维红外光谱中观察到的ν(a)和ν(s)两条谱带都分裂成两个具有重叠谱带特征的组分,这揭示了在11 < m ≤ 16 μmol kg(-1)时界面处两相(LE和LC)共存。从动态红外光谱获得的同步和异步图谱与平衡图谱非常相似。