Cai Zhi-peng, Du Ya-bing, Zhang Ling, Li Peng-wei, Jia Ting-jian, Mo Yu-jun
Institute of Optics & Photoelectronic Technology, College of Physics and Electronics, Henan University, Kaifeng 475004, China.
Guang Pu Xue Yu Guang Pu Fen Xi. 2008 Sep;28(9):2111-4.
The vibrational spectra of ethyl hexanoate were calculated by the density functional theory (DFT) with B3LYP complex function, diffuse function and polarization function added to heavy atoms and light atoms. On the base of this, the normal Raman spectrum (NRS) and the infrared spectrum (IR) were assigned in detail in the present paper. Comparing the calculated results with the experimental data, the calculated results are in good agreement with the experimental results. The comparison of the experimental Raman and infrared spectra shows that in the experimental Raman spectrum, the strongest bands appear at the frequencies of 2600-3100 cm(-1), while the strongest band is not 1734 cm(-1) but 1444 cm(-1) at the frequencies of 400-2000 cm(-1). The band 1734 cm(-1) attributed to the C=O stretch vibration is the distinctive mark of organic ester compounds, and the band 1444 cm(-1) is related to the symmetric and anti-symmetric scissors vibration of C-H. In the experimental infrared spectrum, the strongest vibrational band is 1739 cm(-1), which is related to C=O stretch vibration; At the frequencies of 400-2000 cm(-1), the relative intensity of the infrared spectrum is distinctively stronger than that of the Raman spectrum, but the relative intensity of infrared spectrum is weaker than that of the Raman spectrum at the frequencies of 2600-3100 cm(-1). In the frequencies of 2600-2800 cm(-1), the vibrational bands 2762 and 2732 cm(-1) do not appear in the experimental spectra, which may originate from two reasons: (1) the weak interaction of molecules. Also, the relative intensity of these vibrational bands is very weak in the experimental spectra, and this may testify that the interaction of molecules is rather weak; (2) the vibrational bands may belong to second order vibrational mode at the frequencies of 2600-2800 cm(-1). The relative intensity of infrared bands is weaker than that of the Raman bands at the frequencies of 2600-2800 cm(-1). At the end, the stronger bands appearing in Raman and infrared experimental spectra are assigned as characteristic marks, respectively. The study on vibrational spectra of ethyl hexanoate molecule may have great application value in detection of liquor flavor, chemical industry and biology fields, providing important reference value for the related basic research field.
采用密度泛函理论(DFT)中的B3LYP复合函数,对己酸乙酯的振动光谱进行了计算,并在重原子和轻原子上添加了弥散函数和极化函数。在此基础上,本文详细归属了其常规拉曼光谱(NRS)和红外光谱(IR)。将计算结果与实验数据进行比较,计算结果与实验结果吻合良好。实验拉曼光谱和红外光谱的对比表明,在实验拉曼光谱中,最强谱带出现在2600 - 3100 cm⁻¹频率处,而在400 - 2000 cm⁻¹频率处,最强谱带不是1734 cm⁻¹而是1444 cm⁻¹。归属于C = O伸缩振动的1734 cm⁻¹谱带是有机酯类化合物的特征峰,1444 cm⁻¹谱带与C - H的对称和反对称剪式振动有关。在实验红外光谱中,最强振动谱带为1739 cm⁻¹,与C = O伸缩振动有关;在400 - 2000 cm⁻¹频率范围内,红外光谱的相对强度明显强于拉曼光谱,但在2600 - 3100 cm⁻¹频率处,红外光谱的相对强度弱于拉曼光谱。在2600 - 2800 cm⁻¹频率范围内,实验光谱中未出现2762和2732 cm⁻¹振动谱带,可能源于两个原因:(1)分子间相互作用较弱。同时,这些振动谱带在实验光谱中的相对强度非常弱,这也证实了分子间相互作用较弱;(2)这些振动谱带可能属于2600 - 2800 cm⁻¹频率处的二级振动模式。在2600 - 2800 cm⁻¹频率处,红外谱带的相对强度弱于拉曼谱带。最后,分别将拉曼光谱和红外光谱实验中出现的较强谱带归属为特征峰。己酸乙酯分子振动光谱的研究在白酒风味检测、化工和生物领域可能具有重要应用价值,为相关基础研究领域提供重要参考依据。