Kudo Sachie, Ogawa Hiromi, Yamakita Eri, Watanabe Shio, Suzuki Toshiyuki, Nakashima Satoru
1 Department of Earth and Space Science, Osaka University, Osaka, Japan.
2 Taki Chemical Co., Ltd., Hyogo, Japan.
Appl Spectrosc. 2017 Jul;71(7):1621-1632. doi: 10.1177/0003702817693855. Epub 2017 Jan 1.
Infrared (IR) microspectroscopy combined with a quartz crystal microbalance (QCM) together with an original relative humidity (RH) control system has been developed for studying water adsorption on a collagen film. The adsorbed water weights measured by QCM are almost similar for wetting and drying processes at 28 ℃, indicating that the collagen film is close to the water adsorption/desorption equilibria. A broad OH + NH stretching band area (3000-3700 cm) in the IR spectra of the collagen film increased linearly with the adsorbed weight until about 1.2 μg/8.0 μg dry collagen film at relative humidity (RH) = 40%, while at higher RH (60%, 80%), the band area deviates from the linear trend to the lower side, due to viscoelasticity and others. The OH + NH band can be simulated by four Gaussian components at 3440, 3330, 3210, and 3070 cm with the relatively constant band areas of 3330 and 3070 cm components due to amide A and B (NH) for increasing and decreasing RH. Bound water (3210 cm component: short H bond) constitutes around 70% of total water (3440 + 3210 cm band areas) at RH = 4.9% but decreases to 23% at RH = 80.3%, where free water (3440 cm component: long H bond) becomes dominant over 70%. The peak shifts of C=O stretching (Amide I) and N-H bending (Amide II) can be understood by increasing hydrogen bonding of water molecules (bound water) bound to peptides at lower RH. The higher wavenumber shifts of CH stretching can be due to the loose binding of water molecules (free water) to aliphatic chains on the collagen surface, especially at higher RH. The present combined QCM-IR method is useful for studying amounts and natures of water adsorbing on biomolecules.
已开发出一种将红外(IR)光谱与石英晶体微天平(QCM)以及原始相对湿度(RH)控制系统相结合的方法,用于研究胶原膜上的水吸附情况。在28℃下,通过QCM测量的吸附水重量在湿润和干燥过程中几乎相似,这表明胶原膜接近水吸附/解吸平衡。胶原膜红外光谱中一个较宽的OH + NH伸缩带区域(3000 - 3700 cm)随着吸附重量线性增加,直到在相对湿度(RH) = 40%时达到约1.2 μg/8.0 μg干胶原膜,而在较高的相对湿度(60%,80%)下,由于粘弹性等原因,带面积偏离线性趋势并向较低侧偏移。OH + NH带可以由四个高斯分量在3440、3330、3210和3070 cm处模拟,其中由于酰胺A和B(NH)导致的3330和3070 cm分量的带面积在相对湿度增加和降低时相对恒定。结合水(3210 cm分量:短氢键)在相对湿度(RH) = 4.9%时占总水(3440 + 3210 cm带面积)的约70%,但在相对湿度(RH) = 80.3%时降至23%,此时自由水(3440 cm分量:长氢键)占主导地位超过70%。在较低相对湿度下,与肽结合的水分子(结合水)的氢键增加,可以解释C = O伸缩(酰胺I)和N - H弯曲(酰胺II)的峰位移。CH伸缩的较高波数位移可能是由于水分子(自由水)与胶原表面脂肪链的松散结合,特别是在较高相对湿度下。目前的QCM - IR联合方法对于研究吸附在生物分子上的水的量和性质很有用。