基于粒度端元模型的烟台市养马岛海域沉积动力及物源解析

汤世凯, 李亨健, 强萌麟, 黎奕宏, 孙韶泽, 殷焘, 于林弘. 基于粒度端元模型的烟台市养马岛海域沉积动力及物源解析[J]. 海洋地质与第四纪地质, 2025, 45(3): 62-71. doi: 10.16562/j.cnki.0256-1492.2024061201
引用本文: 汤世凯, 李亨健, 强萌麟, 黎奕宏, 孙韶泽, 殷焘, 于林弘. 基于粒度端元模型的烟台市养马岛海域沉积动力及物源解析[J]. 海洋地质与第四纪地质, 2025, 45(3): 62-71. doi: 10.16562/j.cnki.0256-1492.2024061201
TANG Shikai, LI Hengjian, QIANG Menglin, LI Yihong, SUN Shaoze, YIN Tao, YU Linhong. Sedimentary dynamics and material source in Yangma Island sea area in Yantai based on grain size end-member model[J]. Marine Geology & Quaternary Geology, 2025, 45(3): 62-71. doi: 10.16562/j.cnki.0256-1492.2024061201
Citation: TANG Shikai, LI Hengjian, QIANG Menglin, LI Yihong, SUN Shaoze, YIN Tao, YU Linhong. Sedimentary dynamics and material source in Yangma Island sea area in Yantai based on grain size end-member model[J]. Marine Geology & Quaternary Geology, 2025, 45(3): 62-71. doi: 10.16562/j.cnki.0256-1492.2024061201

基于粒度端元模型的烟台市养马岛海域沉积动力及物源解析

  • 基金项目: 山东省财政项目“山东省烟台市养马岛及邻近海域综合地质调查”(鲁勘字(2023)38号);烟台市财政项目“烟台市城市地质调查(综合成果编制与数据整合建库部分)”(SDGP370600000202302000134)
详细信息
    作者简介: 汤世凯(1988—),男,硕士研究生,高级工程师,研究方向为海岸带地质与海岸沉积,E-mail:tsktop@163.com
    通讯作者: 殷焘(1985—),男,正高级工程师,研究方向为海洋地质勘查及科学研究,E-mail:397921601@qq.com
  • 中图分类号: P736.2

Sedimentary dynamics and material source in Yangma Island sea area in Yantai based on grain size end-member model

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  • 基于养马岛海域30个表层沉积物粒度测试数据,计算沉积物粒度参数、分解粒度端元,结合区域水动力、岸线类型等因素对沉积物的沉积动力环境和物质来源解析判别。结果表明,海域沉积物平均粒径Φ值从河流入海口向远离岸线方向逐渐变大,分选性由中等逐渐变差,偏度以极正偏为主,峰度为中等—尖锐。粒度数据中提取出4个单峰端元组分,EM1、EM2、EM3和EM4粒级Φ值范围分别为2.75~8.75、3.00~6.25、2.25~4.25和1.50~3.75,EM1端元代表了水深较深、水动力弱沉积环境,物源是黄海沿岸流携带的黄河入海泥沙细粒物质;EM2端元代表了潮流波浪叠加作用下水动力较弱的沉积环境,物源是黄海沿岸流携带的黄河入海泥沙与海水侵蚀基岩海岸产生碎屑的混合物质;EM3端元为潮流、波浪叠加和航道影响下水动力较强的沉积环境,物源是入海河流携带泥沙混合海水侵蚀砂、泥岸线的碎屑。EM4端元代表了水深浅,海水与河水动力共同作用下强水动力沉积环境,物源为入海河流携带泥沙混合海水侵蚀砂、泥岸线以及人类活动产生的碎屑。

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  • 图 1  研究区及取样点位置示意图

    Figure 1. 

    图 2  沉积物粒度参数等值线图

    Figure 2. 

    图 3  端元数线性相关和角度离差

    Figure 3. 

    图 4  各端元粒度自然频率分布曲线

    Figure 4. 

    图 5  粒度端元含量等值线分布图

    Figure 5. 

    图 6  沉积动力三角图投点结果

    Figure 6. 

    图 7  沉积物源及物质运移方向示意图

    Figure 7. 

    表 1  沉积物粒度参数及端元含量

    Table 1.  grain size parameters and end member content of sediments

    样品编号 平均粒径/Φ 分选系数 偏度 峰度 端元含量/%
    EM1 EM2 EM3 EM4
    HB1 4.55 1.35 0.47 1.17 29.00 30.81 40.19 0.00
    HB2 4.32 1.69 0.23 1.24 35.54 23.39 29.27 11.81
    HB3 4.74 1.51 0.34 0.98 44.44 23.00 29.87 2.69
    HB4 4.44 1.59 0.27 1.13 36.37 25.21 28.15 10.28
    HS5 5.31 1.41 0.41 0.89 48.80 49.88 1.32 0.00
    HS6 4.94 1.16 0.38 1.10 37.21 60.40 2.39 0.00
    HB7 4.57 1.33 0.32 1.25 29.47 42.56 23.37 4.60
    HB8 4.64 1.29 0.48 1.18 26.32 40.06 33.62 0.00
    HB9 4.35 1.18 0.47 1.30 21.42 31.60 46.97 0.00
    HB10 4.26 1.37 0.30 1.17 28.59 26.79 33.53 11.09
    HS11 4.40 1.20 0.49 1.13 26.08 23.84 50.08 0.00
    HS12 4.94 0.97 0.34 1.20 34.96 65.04 0.00 0.00
    HB13 4.99 1.44 0.37 0.90 45.23 30.39 24.37 0.00
    HB14 4.59 1.26 0.44 1.23 26.27 43.02 30.70 0.00
    HB15 4.44 1.04 0.42 1.36 14.35 55.97 29.69 0.00
    HB16 4.50 1.33 0.32 1.18 32.21 35.73 28.14 3.92
    HS17 4.64 1.05 0.28 1.23 28.06 58.87 13.07 0.00
    HS18 4.87 1.27 0.32 1.02 41.31 40.75 17.94 0.00
    HB19 4.94 1.44 0.21 0.88 55.56 21.54 21.56 1.33
    HB20 4.61 1.23 0.38 1.08 31.08 41.60 26.94 0.37
    HB21 4.28 1.20 0.36 1.51 17.11 40.60 37.79 4.51
    HS22 3.40 1.51 0.74 1.13 16.68 10.31 0.00 73.01
    HS23 4.78 1.33 0.56 1.11 24.20 46.24 29.56 0.00
    HB24 4.27 1.01 0.46 1.63 6.76 50.35 42.89 0.00
    HB25 3.92 0.84 0.19 1.66 1.98 41.31 53.20 3.51
    HB26 2.35 0.34 0.02 0.94 0.00 0.00 0.00 100.00
    HB27 2.71 0.93 0.58 1.58 6.10 10.05 3.95 79.89
    HB28 3.04 0.56 0.16 0.87 0.00 0.00 50.65 49.35
    HB29 5.02 1.83 0.09 0.79 63.37 8.67 14.58 13.39
    HB30 3.60 1.67 0.11 0.99 27.91 26.07 14.16 31.86
    下载: 导出CSV

    表 2  沉积物端元拟合结果

    Table 2.  End member fitting results of sediments

    端元个数端元相关系数R2角度离差
    10.52135.7
    20.83919.9
    30.92013.8
    40.95510.3
    50.9767.4
    60.9904.9
    70.9943.7
    80.9953.4
    90.9952.7
    100.9972.6
    下载: 导出CSV
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出版历程
收稿日期:  2024-06-12
修回日期:  2024-09-06
刊出日期:  2025-06-28

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