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瓦斯浓度影响下水合物晶体结构Raman光谱特征
引用本文:张保勇,周泓吉,吴强,高霞. 瓦斯浓度影响下水合物晶体结构Raman光谱特征[J]. 光谱学与光谱分析, 2016, 36(1): 104-108. DOI: 10.3964/j.issn.1000-0593(2016)01-0104-05
作者姓名:张保勇  周泓吉  吴强  高霞
作者单位:1. 黑龙江科技大学安全工程学院,黑龙江 哈尔滨 150022
2. 瓦斯等烃气输运管网安全基础研究国家级专业中心实验室,黑龙江 哈尔滨 150022
3. 黑龙江科技大学建筑工程学院,黑龙江 哈尔滨 150022
基金项目:国家自然科学基金项目(51334005,51174264,51104062,51274267),黑龙江省普通高等学校青年学术骨干支持计划项目资助
摘    要:在初始温压2 ℃,5 MPa条件下开展了三种瓦斯混合气(CH4—C2H6—N2,G1=54∶36∶10,G2=67.5∶22.5∶10,G3=81∶9∶10)水合实验,利用可见显微拉曼光谱仪获取水合产物拉曼光谱,通过水合物相中C2H6 C—C键伸缩振动特征峰拉曼位移判断水合物晶体结构,利用谱图特征峰分峰拟合方法计算出瓦斯水合物孔穴占有率、水合指数等。研究发现:气样G1和G2水合产物为I型水合物、G3为Ⅱ型,气样中C2H6浓度改变导致水合物晶体结构转变;Ⅰ型结构水合物相中CH4和C2H6含量受气样浓度影响较小,G1和G2体系中CH4含量分别为34.4%和35.7%、C2H6含量分别为64.6%和63.9%,而G3体系中CH4和C2H6含量分别为73.5%和22.8%,晶体结构对水合物相客体分子含量控制作用明显;G1~G3体系水合物相大孔穴的CH4—C2H6占有率分别为98%,98%和92%,小孔穴的CH4占有率分别为80%,60%和84%,N2由于分压较低且吸附能力较弱其小孔穴占有率不高于5%。

关 键 词:瓦斯水合物  拉曼光谱  孔穴占有率  水合指数   
收稿时间:2014-08-21

Raman Characterization of Hydrate Crystal Structure Influenced by Mine Gas Concentration
ZHANG Bao-yong,ZHOU Hong-ji,WU Qiang,GAO Xia. Raman Characterization of Hydrate Crystal Structure Influenced by Mine Gas Concentration[J]. Spectroscopy and Spectral Analysis, 2016, 36(1): 104-108. DOI: 10.3964/j.issn.1000-0593(2016)01-0104-05
Authors:ZHANG Bao-yong  ZHOU Hong-ji  WU Qiang  GAO Xia
Affiliation:1. Department of Safety Engineering, Heilongjiang University of Science and Technology, Harbin 150022, China2. National Central Laboratory of Hydrocarbon Gas Transportation Pipeline Safety, Harbin 150022, China3. School of Architecture and Civil Engineering,Heilongjiang University of Science and Technology, Harbin 150022, China
Abstract:CH4/C2 H6/N2 mixed hydrate formation experiments were performed at 2 ℃ and 5 MPa for three different mine gas concentrations (CH4/C2 H6/N2 ,G1= 54∶36∶10 ,G2= 67.5∶22.5∶10 ,G3= 81∶ 9∶ 10) .Raman spectra for hydration products were obtained by using Microscopic Raman Spectrometer .Hydrate structure is determined by the Raman shift of sym‐metric C-C stretching vibration mode of C2 H6 in the hydrate phase .This work is focused on the cage occupancies and hydration numbers ,calculated by the fitting methods of Raman peaks .The results show that structure Ⅰ (sⅠ ) hydrate forms in the G1 and G2 gas systems ,while structure Ⅱ (sⅡ ) hydrate forms in the G3 gas system ,concentration variation of C2 H6 in the gas samples leads to a change in hydrate structure from sⅠ to sⅡ ;the percentages of CH4 and C2 H6 in sⅠ hydrate phase are less affected by the concentration of gas samples ,the percentages of CH4 are respectively 34.4% and 35.7% ,C2 H6 are respectively 64.6% and 63.9% for gas systems of G1 and G2 ,the percentages of CH4 and C2 H6 are respectively 73.5% and 22.8% for gas systems of G3 ,the proportions of object molecules largely depend on the hydrate structure ;CH4 and C2 H6 molecules occupy 98% ,98% and 92% of the large cages and CH4 molecules occupy 80% ,60% and 84% of the small cages for gas systems of G1 ,G2 and G3 ,respectively ;additionally ,N2 molecules occupy less than 5% of the small cages is due to its weak adsorption ability and the lower partial pressure .
Keywords:Gas hydrate  Raman spectroscopy  Cage occupancies  Hydration number
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