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Four cylindrical sandstone samples were extracted from the original rectangular sample with a rough-walled fracture. Each drilling angle (θ) of cylindrical sandstone samples is different to consider the anisotropies of rough-walled rock fractures. For each sample, different flow velocities ranging from 0 m/s to 13 m/s were designed. For a given flow velocity, a series of different confining pressures ( σ n ), including 1.5 MPa, 2.5 MPa, and 3.5 MPa, were applied on the fractured samples. The hydraulic properties of each cylindrical sandstone sample were tested under different shear displacements ( u s ) and σ n . The results show that the hydraulic gradient ( J ) shows an increasing trend with the increment of σ n . With the increment of the Reynolds number ( Re ), the transmissivity ( T ) decreases in the form of the quadratic function. The normalized transmissivity ( T / T 0 ) decreases with the increment of J . The variations in T / T 0 with J can be divided into three stages. The first stage is that T / T 0 approximately holds a constant value of 1.0 when J is small indicating that the fluid flow is in the linear regime. The last two stages are that T / T 0 decreases with the continuous increase of J , and the reduction rate first increases and then decreases. The critical Reynolds’ number ( Re c ) of the sample angle with a drilling angle of 90° is different from that of other samples. The corresponding Re c is 6.52, 28.73, and 32.1 when the shear displacement u s = 2 mm , 3 mm, and 4 mm, respectively. The variations in Re c and J along different drilling angles are significantly obvious. When the confining pressure is large, the effect of anisotropy on Rec is much greater than that of confining pressure.
Four cylindrical sandstone samples were extracted from the original rectangular sample with a rough-walled fracture. Each drilling angle (θ) of cylindrical sandstone samples is different to consider the anisotropies of rough-walled rock fractures. For each sample, different flow velocities ranging from 0 m/s to 13 m/s were designed. For a given flow velocity, a series of different confining pressures ( σ n ), including 1.5 MPa, 2.5 MPa, and 3.5 MPa, were applied on the fractured samples. The hydraulic properties of each cylindrical sandstone sample were tested under different shear displacements ( u s ) and σ n . The results show that the hydraulic gradient ( J ) shows an increasing trend with the increment of σ n . With the increment of the Reynolds number ( Re ), the transmissivity ( T ) decreases in the form of the quadratic function. The normalized transmissivity ( T / T 0 ) decreases with the increment of J . The variations in T / T 0 with J can be divided into three stages. The first stage is that T / T 0 approximately holds a constant value of 1.0 when J is small indicating that the fluid flow is in the linear regime. The last two stages are that T / T 0 decreases with the continuous increase of J , and the reduction rate first increases and then decreases. The critical Reynolds’ number ( Re c ) of the sample angle with a drilling angle of 90° is different from that of other samples. The corresponding Re c is 6.52, 28.73, and 32.1 when the shear displacement u s = 2 mm , 3 mm, and 4 mm, respectively. The variations in Re c and J along different drilling angles are significantly obvious. When the confining pressure is large, the effect of anisotropy on Rec is much greater than that of confining pressure.
Cohesion and friction angle are important indicators of shear strength in mining engineering. Indoor testing methods are detached from the actual state of the rock mass and affected by disturbances and significant dimensional effects that do not fully reflect the shear strength of the rock mass itself. In situ borehole shear testing is of great practical importance because of its low disturbance and high speed. In this paper, a new testing device based on the principle of a rock borehole shear tester was designed to simulate the shear test in the laboratory. Seven shear indenters were designed to test the effect of different tooth heights, spacing, and angles on the shear strength of rock-like specimens, and the damage surface was scanned in three dimensions and compared with conventional triaxial tests and compression shear tests. The results show that as the tooth height increases, the flatness of the press-in damage surface increases, and the results will be closer to the press-shear test. As the spacing increases, the maximum damage angle and the damage surface between the grooves gradually decrease. The tooth angle has little effect on the friction angle, but cohesion decreases significantly when exceeds 60°.
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