首页 | 本学科首页   官方微博 | 高级检索  
     检索      

正构二十四烷裂解成气碳同位素动力学模拟及其地质意义
引用本文:靳永斌,肖贤明,唐永春,田辉,张同伟.正构二十四烷裂解成气碳同位素动力学模拟及其地质意义[J].沉积学报,2009,27(3):537-545.
作者姓名:靳永斌  肖贤明  唐永春  田辉  张同伟
作者单位:中国科学院广州地球化学研究所 广州 510640
基金项目:国家杰出青年科学基金,中国科学院知识创新工程项目 
摘    要:以甲烷的量子化模型及正构二十四烷(n C24)金管限定体系裂解成气实验为基础,从理论上进一步论述了量子化模型应用于重烃气体(乙烷和丙烷)碳同位素动力学模拟的适应性,计算了甲烷、乙烷及丙烷生烃动力学与碳同位素动力学参数, 重点探讨了δ13C2与δ13C3变化的主控因素。研究结果表明, n C24裂解生成的气态烃碳同位素与早期报道的n C18、n C25及原油裂解生成的气态烃碳同位素具有可比性,可应用于地质条件下解释原油裂解气的某些地球化学特征。n C24生烃地质模型表明,其在150~160℃是稳定的,主要裂解温度介于180~200℃之间,与目前所报道的原油裂解地质模型吻合。随热解程度的增加,δ13C2与δ13C3体现了比δ13C1更明显的变化。气藏充注历史控制的同位素累积效应对天然气碳同位素有很大的影响,与累积聚集气相比,阶段聚集气的δ13C变重,并在更大程度上影响了演化曲线的分异。在此基础上,应用n C24裂解成气碳同位素分馏地质模型探讨了塔里木盆地某些油气藏天然气碳同位素值变化的原因。

关 键 词:正构二十四烷    裂解成气    重烃气体    碳同位素动力学
收稿时间:1900-01-01

A Kinetic Model of Stable Carbon Isotope Ratios in Gaseous Hydrocarbons Generated from Thermal Cracking of n-tetracosane and Its Geological Significance
JIN Yong-bin,XIAO Xian-ming,TANG Yong-chun,TIAN Hui,ZHANG Tong-wei.A Kinetic Model of Stable Carbon Isotope Ratios in Gaseous Hydrocarbons Generated from Thermal Cracking of n-tetracosane and Its Geological Significance[J].Acta Sedimentologica Sinica,2009,27(3):537-545.
Authors:JIN Yong-bin  XIAO Xian-ming  TANG Yong-chun  TIAN Hui  ZHANG Tong-wei
Institution:State Key Laboratory of Organic Geochemistry, Guangzhou Institute of Geochemistry, Chinese Academy of Sciences, Wushan Guangzhou 510640
Abstract:Based on quantitative modeling and experimental data on n tetracosane cracking to generate gaseous hydrocarbons in a confined system, we calculated the generation kinetics and carbon isotope kinetics of methane, ethane and propane and determined the main controlling factors influencing the variation of δ13C2 and δ13C3. The carbon isotope of gaseous hydrocarbons from nC24 cracking to gas are comparable to those from crude oil reported recently, and they can be used to investigate the geochemical characteristics of crude oil cracking to gas under geological conditions. The geological model of nC24 cracking suggests it is stable at 150~160℃ and its cracking temperature ranges 180℃ to 200℃, consistent with geological models of crude oil cracking currently reported. With increasing degree of thermal stress, the changes in δ13C2 and δ13C3 are larger than that of δ13C1. It is shown that isotope accumulation controlled by the recharging history of a reservoir has a considerable impact on the carbon isotope distribution of natural gas. Compared to that of cumulative gas, the carbon isotope ratio of partly accumulation gas is heavier and influences the fractionation of the δ13C2 and δ13C3 curves to a greater extent. The geological model of nC24 cracking to gas has been used to interpret the origin of carbon isotopic variation of natural gas in some reservoirs in the Tarim basin.
Keywords:n-tetracosane  crude oil cracking gas  heavy hydrocarbon gas  carbon isotopic kinetics  
本文献已被 CNKI 万方数据 等数据库收录!
点击此处可从《沉积学报》浏览原始摘要信息
点击此处可从《沉积学报》下载免费的PDF全文
设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号