冷泉活动区气泡羽状流数值模型研究

李灿苹, 勾丽敏, 尤加春, 欧触灵. 冷泉活动区气泡羽状流数值模型研究[J]. 海洋地质与第四纪地质, 2017, 37(5): 141-150. doi: 10.16562/j.cnki.0256-1492.2017.05.014
引用本文: 李灿苹, 勾丽敏, 尤加春, 欧触灵. 冷泉活动区气泡羽状流数值模型研究[J]. 海洋地质与第四纪地质, 2017, 37(5): 141-150. doi: 10.16562/j.cnki.0256-1492.2017.05.014
LI Canping, GOU Limin, YOU Jiachun, OU Chuling. STUDY ON NUMERICAL MODELS ABOUT BUBBLE PLUMES IN THE COLD SEEPAGE ACTIVE REGION[J]. Marine Geology & Quaternary Geology, 2017, 37(5): 141-150. doi: 10.16562/j.cnki.0256-1492.2017.05.014
Citation: LI Canping, GOU Limin, YOU Jiachun, OU Chuling. STUDY ON NUMERICAL MODELS ABOUT BUBBLE PLUMES IN THE COLD SEEPAGE ACTIVE REGION[J]. Marine Geology & Quaternary Geology, 2017, 37(5): 141-150. doi: 10.16562/j.cnki.0256-1492.2017.05.014

冷泉活动区气泡羽状流数值模型研究

  • 基金项目:
    国家自然科学基金项目(41306050);中央高校基本科研业务费专项(2652013122);广东省科技计划项目(2014A010103030);广东省自然科学基金(2015A030313617)
详细信息
    作者简介: 李灿苹(1977—),女,副教授,主要从事天然气水合物地震勘探数值模拟研究,E-mail: canpinglihydx@163.com
    通讯作者: 勾丽敏(1972—),女,讲师,主要从事地震资料处理及散射波地震勘探研究,E-mail:goulm@163.com
  • 中图分类号: P738

  • 蔡秋蓉编辑

STUDY ON NUMERICAL MODELS ABOUT BUBBLE PLUMES IN THE COLD SEEPAGE ACTIVE REGION

More Information
  • 羽状流对天然气水合物的识别起到了间接指示作用,为研究冷泉活动区气泡羽状流产生的地震响应,需建立符合实际羽状流特征的模型。为此,参考实际羽状流赋存状态,结合含气泡水体特征,在已建立模型基础上,从羽状流气泡的垂直运移规律、分布特点及羽状流外观特征上对模型进行了改进,先后获得3个羽状流模型,最后的模型Ⅲ更接近实际羽状流赋存特征。通过与实际羽状流的对比,讨论分析了模型Ⅲ的合理性,并得出结论:所建模型体现了实际羽状流气泡的本质特征,并包含了更为复杂的气泡含量变化,可用于进一步深入研究羽状流地震响应特征,也为气泡羽状流的地震识别及天然气水合物的相关研究提供了较好的数值模型。

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  • 图 1  我国南海某测区羽状流地震偏移剖面

    Figure 1. 

    图 2  羽状流模型建立流程图

    Figure 2. 

    图 3  羽状流模型Ⅰ[24]

    Figure 3. 

    图 4  鄂霍次克海冷泉气泡羽状流[10]

    Figure 4. 

    图 5  重构的羽状流模型(模型Ⅱ)[26]

    Figure 5. 

    图 6  不同倾斜角度的羽状流水体模型

    Figure 6. 

    图 7  模型Ⅲ垂直形状、一个周期的羽状流水体模型

    Figure 7. 

    图 8  模型Ⅲ(图 7)第50炮地震记录

    Figure 8. 

    图 9  模型Ⅲ(图 7)偏移叠加剖面

    Figure 9. 

    图 10  挪威斯瓦尔巴特群岛气泡羽状流声呐图[37]

    Figure 10. 

    表 1  声速表达式(1)中各参数说明

    Table 1.  Explanation of parameters in equation (1) of acoustic velocity

    参量 参量含义 取值 单位
    Cm 气液混合物的声波速度 - m/s
    K 液体体积模量 2.34×109 N/m3
    Kb 气体体积模量 1.4×105 N/m3
    ρ 液体密度 1 023 kg/m3
    ρb 气体密度 1.29 kg/m3
    ω 频率 25 KHz
    a 气泡半径 - m
    σ 液体表面张力 0.073 8 N/m3
    R 假定含气泡两相混合区
    为球形时的半径
    1.0 m
    φ 气泡含量(体积分数) - -
    下载: 导出CSV

    表 2  正演模拟采集参数

    Table 2.  Acquisition parameters of forward simulation

    测线长度/m 深度/m 网格剖分 震源主频/Hz 炮间距/m 总炮数 炮点深度/m 道间距/m 排列长度/m 最小偏移距/m 记录长度/s 采样率/ms
    1 000 400 1 m×1 m 140 10 101 0 1 1 000 0 1.6 0.2
    下载: 导出CSV
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出版历程
收稿日期:  2017-06-01
修回日期:  2017-07-03
刊出日期:  2017-10-28

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