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渤中19-6孔店组砂砾岩孔隙结构和渗透率估算模型

宋晨 杨兵 张超谟 朱博远 张占松

宋晨, 杨兵, 张超谟, 朱博远, 张占松. 渤中19-6孔店组砂砾岩孔隙结构和渗透率估算模型[J]. 地质科技通报, 2023, 42(1): 274-285. doi: 10.19509/j.cnki.dzkq.2022.0093
引用本文: 宋晨, 杨兵, 张超谟, 朱博远, 张占松. 渤中19-6孔店组砂砾岩孔隙结构和渗透率估算模型[J]. 地质科技通报, 2023, 42(1): 274-285. doi: 10.19509/j.cnki.dzkq.2022.0093
Song Chen, Yang Bing, Zhang Chaomo, Zhu Boyuan, Zhang Zhansong. Investigation of pore structure and permeability estimation models of Kongdian Formation glutenites in the Bozhong 19-6 Gasfield[J]. Bulletin of Geological Science and Technology, 2023, 42(1): 274-285. doi: 10.19509/j.cnki.dzkq.2022.0093
Citation: Song Chen, Yang Bing, Zhang Chaomo, Zhu Boyuan, Zhang Zhansong. Investigation of pore structure and permeability estimation models of Kongdian Formation glutenites in the Bozhong 19-6 Gasfield[J]. Bulletin of Geological Science and Technology, 2023, 42(1): 274-285. doi: 10.19509/j.cnki.dzkq.2022.0093

渤中19-6孔店组砂砾岩孔隙结构和渗透率估算模型

doi: 10.19509/j.cnki.dzkq.2022.0093
基金项目: 

国家科技重大专项 2017ZX05032-003-005

详细信息
    作者简介:

    宋晨(1997—),女,现正攻读矿物学、岩石学、矿床学专业硕士学位,主要从事地球物理研究工作。E-mail: 390172641@qq.com

    通讯作者:

    张超谟(1962—),男,教授,主要从事地球物理测井研究工作。E-mail: zhang7801@263.cn

  • 中图分类号: TE122.23

Investigation of pore structure and permeability estimation models of Kongdian Formation glutenites in the Bozhong 19-6 Gasfield

  • 摘要:

    渤中19-6砂砾岩孔隙结构复杂,为提高渗透率的估算精度,需要从孔隙结构入手,找到与渗透率相关性最好的孔隙结构因素。以43块孔店组砂砾岩的孔隙结构和渗透率为研究对象,利用岩石铸体薄片确定发育的孔隙类型,通过高压压汞获取孔喉分布特征和孔隙结构参数。结合孔隙类型和孔隙结构参数分析孔隙结构和渗透率的关系,建立了基于孔隙结构参数的渗透率评价模型。研究表明,不同类型溶蚀孔隙的孔隙结构存在差异,粒内溶孔的孔隙结构最好,胶结物溶孔的孔隙结构最差。溶蚀孔隙类型发育不同,物性差异较大,以粒内溶孔为主且不发育胶结物溶孔的岩样物性最好。不同孔隙结构因素对渗透率控制程度不一致,其中基于孔喉大小、连通、配比和几何形状这4种因素建立的渗透率模型精度最高。渤中19-6气田孔店组砂砾岩粒内溶孔具有较大的孔喉半径和较好的连通性是促使该类岩石储集和渗流能力均较好的主要原因。平均孔喉半径、退汞效率、平均孔喉体积比和分形维数适用于估算孔隙结构复杂且(特)低孔渗的砂砾岩储层渗透率,以期为渤海湾盆地渤中凹陷砂砾岩储层的渗透率评价提供技术支持。

     

  • 图 1  渤中19-6构造带位置[26]及砂砾岩储层岩性

    Figure 1.  Location of Bozhong 19-6 structural belt and lithology of glutenite reservoirs

    图 2  恒速毛管压力进汞及进汞过程压力涨落

    1~4.孔隙序号;Ⅰ~Ⅳ.压力降落等级;a~d.孔隙1~4的体积;e~f.喉道连接体积;rison.一个独立的喉道总是存在一个半径最小的截面,在汞到达这个最小截面之前毛管压力不断上升的过程; rhcon.汞突破最小的喉道进入较大喉道中所引起毛管压力突降的现象; subisou.在进汞压力未超过rhcon发生之前的压力时的过程

    Figure 2.  Pressure rises and falls during mercury intrusion and the mercury with drawal process

    图 3  孔隙度与渗透率交会图和不同类型样品的物性特征

    Figure 3.  Cross-plot of porosity versus permeability and different types of porosity and permeability

    图 4  铸体薄片观察的典型孔隙类型

    a.1#,3 850.85 m,主要见粒内溶孔、胶结物溶孔和粒间溶孔;b.2#,4 050.5 m,主要见粒间溶孔、粒内溶孔和颗粒裂隙;c.3#,3 856.15 m,主要见粒内溶孔、粒间溶孔和颗粒裂隙;d.4#,3 850.47 m,主要见粒内溶孔、高岭石溶孔、粒间溶孔和颗粒裂隙;e.5#,4 047.63 m,主要见粒间溶孔、粒内溶孔;f.6#,3 856.84 m,主要见粒内溶孔、颗粒裂隙和粒间溶孔

    Figure 4.  Typical pore types observed in the thin sections

    图 5  从压汞数据获得的样品孔喉分布

    Figure 5.  Pore-throat size distribution obtained from high-pressure mercury injection

    图 6  压汞曲线和孔喉分布特征

    Figure 6.  Mercury injection curve and pore-throat size distribution characteristics

    图 7  孔隙结构影响渗流能力的机制示意图

    Figure 7.  Schematic diagram of the mechanism of pore structure affecting seepage capacity

    图 8  孔隙结构参数和渗透率的关系

    Figure 8.  Relationship between pore structure parameters and permeability

    图 9  不同渗透率模型估算渗透率与测试渗透率交会图

    Figure 9.  Cross-plot of the estimated and measured permeabilities for each permeability model

    图 10  孔隙结构对渗透率的控制程度

    Figure 10.  Effect of pore structure on permeability

    表  1  孔隙结构参数意义和分类

    Table  1.   Pore structure parameters and its physical meaning

    符号 孔隙结构参数 物理意义 表示信息 参数计算方法
    Rave 平均孔喉半径/μm[6] 衡量岩石的平均孔喉大小,反映物性好坏。其越大,储层物性越好 孔喉大小 $\sqrt{\left(\sum\limits_1^n r_i^{\prime 2} \cdot S_{\mathrm{hg}}\right) / \sum\limits_1^n \Delta S_{\mathrm{hg}}}$
    Rapex Swanson半径/μm[7, 18] 岩石内部无效孔隙向有效连通的孔隙系统过渡时的孔喉半径大小,反映对流体流动作出贡献的有效孔隙空间的体积 孔喉大小 Shg/Pc的最大值所对应的孔喉半径
    Sp 分选系数[8] 反映孔喉分布的分选性(集中程度),表示以Rave为中心的散布程度。高渗储层分选越好,渗流能力越强。低渗储层分选越差,渗流能力越强 孔喉分布 $\sqrt{\left[\sum\limits_1^n\left(r^{\prime}{ }_i-R_{\mathrm{ave}}\right)^2 \cdot \Delta S_{\mathrm{hg}}\right] / \sum\limits_1^n \Delta S_{\mathrm{hg}}}$
    We 退汞效率/%[9] 反映孔隙通过喉道相连接的墨水瓶现象。其越低,喉道对孔隙的控制作用越强,首先退出汞的喉道对孔隙空间连通性造成的破坏越大,渗流能力越差 孔喉连通 $\frac{S_{\max }-S_{\mathrm{r}}}{S_{\max }}$
    Rpt 平均孔喉体积比[10] 反映储集空间中孔隙和喉道的平均体积比。其越大,与孔隙相连的喉道半径越小,流体在孔隙空间中流动越容易发生卡断,不能形成连续相,渗流能力越差 孔喉配比 $\frac{{{S_{\rm{r}}}}}{{{S_{\max }} - {S_{\rm{r}}}}}$
    Df 分形维数[5] 刻画孔喉几何形体复杂程度的定量参数。分形维数越大,孔隙和喉道的非均质性越强,渗流能力越差 孔喉几何 ${S_{{\rm{hg}}}} \propto P_{\rm{c}}^{ - \left( {2 - {D_{\rm{f}}}} \right)}$
      注:r′i为某一进汞区间孔喉半径中值(μm);ΔShgri对应区间进汞饱和度增量(%);Sr为残余汞饱和度(%);Smax为最大汞饱和度(%)
    下载: 导出CSV

    表  2  6块样品的孔渗和孔隙结构参数

    Table  2.   Porosity, permeability and pore structure parameters of the 6 samples

    样品 深度/m 孔隙度/% 渗透率/10-3 μm2 孔隙结构参数
    Rave/μm Rapex/μm Sp We/% Rpt Df
    1# 3 850.84 9.80 0.05 0.373 0.720 0.641 19.610 4.099 2.276
    2# 4 050.49 9.50 1.89 1.022 1.572 0.777 34.600 1.890 2.109
    3# 3 856.16 9.90 2.41 1.288 2.237 1.203 35.808 1.793 2.104
    4# 3 850.45 10.50 0.54 0.922 1.101 0.684 25.221 2.965 2.157
    5# 4 047.65 10.60 1.74 0.825 1.564 0.745 36.966 1.705 2.124
    6# 3 856.85 10.70 2.57 1.308 2.216 1.110 35.970 1.780 2.096
    下载: 导出CSV

    表  3  考虑不同个数因素回归的渗透率模型以及相关性、均方根误差

    Table  3.   Permeability model considering the different factors, correlation coefficient and RMSE

    模型编号 考虑因素 R2 均方根误差 回归模型
    1 Df 0.627 6 0.876 1 lgK=15.457-46.765·lgDf
    2 Df, We 0.626 1 0.873 0 lgK=14.071-45.121·lgDf+0.556·lgWe
    3 Df, We, Rpt 0.633 8 0.865 6 lgK=17.860-1.401·lgRpt-45.856·lgDf-1.503·lgWe
    4 Df, We, Rpt , Rave 0.894 2 0.507 7 lgK=-11.595+1.809·lgRave+4.942·lgRpt-9.174·lgDf+8.720·lgWe
    5 Df, We, Rpt, Rapex 0.845 5 0.613 7 lgK=3.142+1.110·lgRapex+1.919·lgRpt-28.473·lgDf+3.618·lgWe
    6 Df, We, Rpt, Rave, Sp 0.889 1 0.527 0 lgK=-8.273+0.944·lgRave+4.770·lgRpt-17.596·lgDf+8.397·lgWe+0.667·lgSp
    7 Df, We, Rpt, Rave, Sp, φ 0.830 7 0.649 1 lgK=-6.527+0.631·lgRave+4.266·lgRpt-21.573·lgDf+7.655·lgWe+0.574·lgSp+0.828·lgφ
    下载: 导出CSV

    表  4  几种常用的压汞孔隙结构参数渗透率模型

    Table  4.   Several common permeability models built by pore structure parameters

    常用回归模型 模型关键参数 岩性 渤中19-6回归公式 R2 均方根误差
    Winland[22] φR35 碎屑砂岩 lgK=-0.662+0.988·lgφ+0.646·lgR35 0.742 8 0.755 7
    Swanson[18] Shg/Pc 砂岩,碳酸盐岩 lgK=-2.767+1.767·lg(Shg/Pc)max 0.777 6 0.864 4
    Pittman[20] φR25 砂岩 lgK=-0.577+0.621·lgφ+1.128·lgR25 0.792 9 0.703 9
    Capillary-Parachor[19] Shg/Pc2 砂岩 lgK=-1.795+0.896·lg(Shg/Pc2)max 0.757 7 0.775 8
    Rezaee[35] φR50 碳酸盐岩 lgK=-2.236+2.611·lgφ+0.151·lgR50 0.709 5 0.806 5
    Rezaee[21] φR10 致密砂岩 lgK=0.825-1.888·lgφ+2.768·lgR10 0.781 3 0.929 4
    Gao and Hu[36] R50 砂岩、页岩 lgK=0.552+0.297·lgR50 0.414 7 1.060 6
    Liu[37] φShg/Pc2 砂岩 lgK=-2.025+0.431·lgφ+0.806lg(Shg/Pc2)max 0.768 7 0.752 9
    本文 RaveRptDfWe 砂砾岩 lgK=-11.595+1.809·lgRave+4.942·lgRpt-9.174·lgDf+8.720·lgWe 0.894 2 0.507 7
      注:R10为进汞饱和度为10%时对应的孔喉半径;R50为进汞饱和度为50%时对应的孔喉半径;R25为进汞饱和度为25%时对应的孔喉半径;Φ为孔隙度
    下载: 导出CSV
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