天然气水合物降压开采分解前缘移动数值研究

彭盈钰, 苏正, 刘丽华, 金光荣, 魏雪芹. 天然气水合物降压开采分解前缘移动数值研究[J]. 海洋地质与第四纪地质, 2020, 40(6): 198-207. doi: 10.16562/j.cnki.0256-1492.2020072701
引用本文: 彭盈钰, 苏正, 刘丽华, 金光荣, 魏雪芹. 天然气水合物降压开采分解前缘移动数值研究[J]. 海洋地质与第四纪地质, 2020, 40(6): 198-207. doi: 10.16562/j.cnki.0256-1492.2020072701
PENG Yingyu, SU Zheng, LIU Lihua, JIN Guangrong, WEI Xueqin. Numerical study on the movement of the decomposition front of natural gas hydrate under depressurization[J]. Marine Geology & Quaternary Geology, 2020, 40(6): 198-207. doi: 10.16562/j.cnki.0256-1492.2020072701
Citation: PENG Yingyu, SU Zheng, LIU Lihua, JIN Guangrong, WEI Xueqin. Numerical study on the movement of the decomposition front of natural gas hydrate under depressurization[J]. Marine Geology & Quaternary Geology, 2020, 40(6): 198-207. doi: 10.16562/j.cnki.0256-1492.2020072701

天然气水合物降压开采分解前缘移动数值研究

  • 基金项目: 2018年广东省促进经济发展专项资金(海洋经济发展用途)“天然气水合物先导区开发潜力分析与评价”(GDME-2018D001-06);2019年省级促进经济发展专项资金项目“水合物开采安全评价预测技术研究”(GDOE[2019]A41);2020年中国科学院南海生态环境工程创新研究院项目“生物礁地球化学记录反演南海沉积环境变化研究”(ISEE2020YB05);2018年广东省海洋科技协同创新中心项目“南海北部台西南盆地浅层沉积物中自生碳酸盐岩形成动力学模拟研究”(20180207)
详细信息
    作者简介: 彭盈钰(1996—),女,硕士研究生,主要从事天然气水合物开采方向研究,E-mail:pengyy@ms.giec.ac.cn
    通讯作者: 苏正(1980—),男,博士,研究员,主要从事天然气水合物成藏机制和开采潜力评价研究,E-mail:suzheng@ms.giec.ac.cn
  • 中图分类号: P738

Numerical study on the movement of the decomposition front of natural gas hydrate under depressurization

More Information
  • 在水合物分解过程中,已经分解的区域与未分解的区域之间存在一个过渡带,即分解前缘,研究分解前缘移动规律有助于认识水合物分解特征和进一步预测分解气量,对实际开采以及开采潜力评价提供大方向的科学参考。本文依据Stefan边界理论建立水合物分解前缘一维三相数学模型,通过参数量级分析,将水合物分解渗流场作为拟定常场,解析计算得到分解前缘随时间移动函数,同时将温度场方程无维化转换后,得到计算温度变化的超越方程。据分解前缘移动函数进一步计算总产气量以及井口产气速率。结合模型算例,认为水合物分解前缘移动与时间的平方根呈线性关系,移动速率随时间推移而减小,产气速率在开采前期达到峰值后快速下降达到稳定值。另外,以南海神狐海域第一次试采结果为依据,对比发现模型计算总气量高于实际试采值,两者相对误差在可接受范围内。因此,本文对水合物开采特征评价提供了一种新的简单计算方法,并对开采潜力给出了乐观的预测。最后,通过对地层初始温度、绝对渗透率以及孔隙度敏感性分析发现,地层初始温度和渗透率增大,水合物分解前缘移动距离随之增大,初始地层温度对水合物分解影响显著。而地层孔隙度越大,分解前缘移动速率反而降低,移动距离减小,井口与分解前缘压差减小,此时分解前缘移动由储层热物理参数决定。

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  • 图 1  天然气水合物开采分解前缘迁移概念模型

    Figure 1. 

    图 2  实验与模型下的分解前缘移动

    Figure 2. 

    图 3  水合物开采特征

    Figure 3. 

    图 4  模型计算总产气量与试采结果对比

    Figure 4. 

    图 5  不同储层初始温度下水合物分解前缘移动距离

    Figure 5. 

    图 6  不同储层绝对渗透率下水合物分解前缘移动距离

    Figure 6. 

    图 7  不同储层孔隙度下水合物分解前缘移动距离

    Figure 7. 

    表 1  初始条件与边界条件

    Table 1.  Initial conditions and boundary conditions

    初边值条件
    初始地层压力(
    初始地层温度(
    井底压力()
    外边界压力()
    外边界温度()
    下载: 导出CSV

    表 2  相关物性参数

    Table 2.  The correlated parameters used for calculation

    参数数值
    水合物密度(kg/m3910
    岩石密度(kg/m32 650
    水合物层厚度h(m)40
    水合物饱和度0.3
    水合物层水饱和度0.7
    孔隙度0.3
    初始地层压力(MPa)14.0
    初始地层温度(K)287.15
    井底压力(MPa)3.0
    单位质量水合物中气体体积分数0.129
    气体运动黏滞系数(Pas)1.e-5
    水相运动黏滞系数(Pas)1.e-3
    水合物层绝对渗透率K(md)2.9
    井筒地层绝对渗透率K(md)150
    水合物分解吸收热(kJ/kg)430
    水合物导热系数(W/mK)2.11
    岩石导热系数(W/mK)2.0
    水导热系数(W/mK)0.58
    水合物比热容(KJ/kg K)2.22
    水比热容(KJ/kg K)4.2
    岩石比热容(KJ/kg K)1.0
    下载: 导出CSV
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出版历程
收稿日期:  2020-07-27
修回日期:  2020-09-01
刊出日期:  2020-12-25

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