日本地球惑星科学連合2025年大会

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[J] 口頭発表

セッション記号 H (地球人間圏科学) » H-SC 社会地球科学・社会都市システム

[H-SC06] 地球温暖化防⽌と地学(CO2地中貯留・有効利⽤、地球⼯学)

2025年5月27日(火) 10:45 〜 12:15 103 (幕張メッセ国際会議場)

コンビーナ:徂徠 正夫(国立研究開発法人産業技術総合研究所 地圏資源環境研究部門)、薛 自求(公益財団法人 地球環境産業技術研究機構)、愛知 正温(東京大学大学院新領域創成科学研究科)、今野 義浩(The University of Tokyo, Japan)、座長:徂徠 正夫(国立研究開発法人産業技術総合研究所 地圏資源環境研究部門)

11:15 〜 11:30

[HSC06-09] せん断増粘流体による岩石の多方向水圧破砕のDEMシミュレーション

*和田 琉1椋平 祐輔2、石原 真吾3渡邉 則昭1、伊藤 高敏2 (1.東北大学大学院環境科学研究科、2.東北大学流体科学研究所、3.東北大学未来科学技術共同研究センター)


キーワード:個別要素法、水圧破砕、せん断増粘流体

The conventional hydraulic fracturing method used in subsurface resource development has a fundamental limitation: it can only induce fractures along the maximum principal stress direction, thereby restricting permeability enhancement to a single orientation. To overcome this limitation, shear thickening fluid (STF) has been proposed as a fracturing fluid (Mukuhira et al., ARMA, 2024), showing its potential to generate multi-directional fractures. STF is a type of non-Newtonian fluid and its viscosity varies with the shear rate; it shows quasi-solid behavior under shear. Laboratory experiments in the previous study have demonstrated multiple pressure build-ups and drops, as well as fractures forming in various directions, which are phenomena absent in conventional hydraulic fracturing. However, the underlying mechanism of these behaviors has not been fully understood due to the limitations of experimental observation. To address this, we conducted numerical simulations using the discrete element method (DEM) to model STF fracturing processes.
In this study, we implemented a shear rate-dependent viscosity function into our in-house 2D DEM code which can simulate hydraulic fracturing. Specifically, we implemented a shear rate-dependent viscosity model, allowing STF viscosity to vary dynamically in response to local flow velocities. Additionally, a relaxation time function was introduced to account for the time-dependent recovery of viscosity.
Simulations were performed using a rock model with a single pre-existing fracture to analyze the effects of STF on pressure variation and fracture propagation. The 2D square rock models had a borehole in the center and the pre-existing fracture set from the borehole to the one boundary of the model. In the calculation, STF and Newtonian fluid were injected into the borehole of each model for comparison, and then borehole pressure variation and subsequent phenomena were observed.
The simulation results demonstrated that STF injection led to higher borehole pressure than the case of Newtonian fluid and an additional fracture generation with a pressure drop. In the case of Newtonian fluid, the borehole pressure linearly increased and then stabilized at a constant level resulting in a steady-state flow condition. Since the fluid just flowed out of the pre-existing fracture, additional fracture generations did not occur in the case of Newtonian fluid. The analysis of the results showed a drastic increase in viscosity around the borehole in the case of STF.
We interpret the results as follows. The increase in viscosity near the borehole reduced the fluid outflow from the borehole into the pre-existing fracture and led to an increase in borehole pressure to a higher value than that of the Newtonian fluid case. Higher borehole pressure may cause additional fracture generation which did not occur in the case of Newtonian fluid.
The simulation results demonstrated our successful implementation of the STF shear thickening effect in our DEM, as well as the qualitative reproduction of STF's quasi-solid behavior. In addition, the results provide insights into the mechanism of multidirectional fracturing by STF, that high viscous STF acted as a seal within fractures, temporarily restricting flow and promoting borehole pressure build-up. Our simulations support the hypothesis in the previous study (Mukuhira et al., ARMA, 2024) that STF viscosity variations play a crucial role in multi-directional fracture propagation.
This study provides new insights into the mechanism of STF fracturing and demonstrates the effectiveness of our modified DEM model. By incorporating a shear rate-dependent viscosity model and relaxation time function, we were able to capture the dynamic behavior of STF and its effects on fracture propagation. Future work will focus on refining the model to reproduce the whole process of STF fracturing and fully understand its mechanism.