非均质条件下弱凝胶分布与运移深度
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国家自然科学基金 “ CO2 微气泡 / 两亲聚合物在稠油化学降黏复合驱中协同作用机制研究 ” (项目编号 52474071)。


Distribution and Migration Depth of Weak Gel under Heterogeneous Condition
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    摘要:

    弱凝胶的分布与运移能力直接影响其调驱效果,常规岩心封堵实验无法直观观测凝胶的分布特征,也较少 反映油藏非均质性对运移过程的影响。本文分别在长填砂模型、大尺寸可视化非均质模型和非均质岩心模型中 开展弱凝胶调驱与 CT 扫描实验,系统研究弱凝胶的空间分布特征与运移深度规律。长填砂模型结果表明:成胶 液达到终凝时间 (12 . 0 ~ 14 . 0 h) 前,动态注入压力已显著升高至最高 37 . 5 MPa,这一方面证实动态成胶过程已发 生,另一方面说明孔隙介质中成胶液在终凝前就已出现运移阻力急剧增大、流动困难的现象,采用终凝时间无法 准确反映成胶液在孔隙介质中的流动性。成胶液注入及后续水驱过程中,弱凝胶虽可发生运移,但运移距离十 分有限 (模型总长 21 . 5 m,成胶阶段弱凝胶仅挤注至 0 ~ 4 . 2 m 段,后续水驱仅可将其推进至 4 . 2 ~ 8 . 5 m 段形成封 堵),且需要 15 . 0 ~ 37 . 5 MPa 的极高顶替压力。可视化非均质模型结果显示:第一轮次弱凝胶的封堵深度约为 27 . 0 cm,后续注水及第二轮、第三轮成胶液注入过程中,注入介质存在明显绕流,注入压力仅小幅升高,前置轮次 凝胶未发生明显运移,还会对后续轮次成胶液的运移产生遮挡;三轮次注入后总封堵深度仅为 43 . 3 cm,远小于 模型总长 200 . 0 cm,证实非均质条件下弱凝胶运移能力极弱甚至基本无法运移。非均质岩心模型的流体分布结 果进一步验证:非均质条件下弱凝胶成胶后基本无法实现有效深部运移,更多发挥 “ 调剖 ” 作用而非 “ 调驱 ” 作用。

    Abstract:

    The distribution and migration ability of weak gel directly affect its profile control and flooding performance. Conventional plugging experiments using core models cannot intuitively observe gel distribution,and rarely reflect the influence of reservoir heterogeneity on migration process. In this paper,weak gel profile control and flooding as well as CT scanning experiments were carried out in long sand filling model,large-size visual heterogeneous model and heterogeneous core model,respectively,to systematically study the spatial distribution and migration depth of weak gel. The results of long sand filling model showed that before reaching final setting time (12 . 0 — 14 . 0 h),the dynamic injection pressure of the gelling fluid had increased significantly to a maximum of 37 . 5 MPa. On the one hand,this confirmed the occurrence of dynamic gelation;on the other hand,it indicated that the migration resistance of gelling fluid increased sharply and flow became difficult before final setting in porous media,so final setting time could not accurately reflect the fluidity of gelling fluid in porous media. During gelling fluid injection and subsequent water flooding,weak gel could migrate,but the migration distance was very limited. The total length of the model was 21 . 5 m;weak gel only was squeezed to 0 — 4 . 2 m section in the gelling stage,and subsequent water flooding could only push it to 4 . 2 — 8 . 5 m section for plugging requiring an extremely high displacement pressure of 15 . 0 — 37 . 5 MPa. The results of visual heterogeneous model showed that the plugging depth of the first round of weak gel was about 27 . 0 cm. During subsequent water injection and the injection of the second and third rounds of gelling fluid,the injected fluid had obvious bypass flow,the injection pressure only increased slightly,the gel of previous rounds did not migrate significantly,and it would also block the migration of subsequent rounds of gelling fluid. After three rounds of injection,the total plugging depth was only 43 . 3 cm,which was far less than the total length of the model (200 . 0 cm),confirming that weak gel had very poor migration ability or even basically could not migrate under heterogeneous conditions. The fluid distribution results of heterogeneous core model further verified that weak gel could basically not achieve effective deep migration after gelation under heterogeneous conditions,and it played more role of “ profile control ” rather than “ profile control and flooding ” .

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薛新房,杨劲舟,王业飞,李 翔,邱世泽,徐国瑞,张俊谦,于 童,丁名臣.非均质条件下弱凝胶分布与运移深度[J].油田化学,2026,43(2):214-220.
XUE Xinfang, YANG Jinzhou, WANG Yefei, LI Xiang, QIU Shize, XU Guorui, ZHANG Junqian, YU Tong, DING Mingchen. Distribution and Migration Depth of Weak Gel under Heterogeneous Condition[J]. OILFIELD CHEMISTRY,2026,43(2):214-220.

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  • 在线发布日期: 2026-08-03
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