Abstract:
In underground excavation and associated stress adjustments, the surrounding rock mass typically experiences non-hydrostatic and deviatoric multi-axial stress conditions. Among the three principal stresses, the intermediate principal stress (
σ2) has been increasingly recognized as a critical factor governing the deformation behavior, crack evolution, and failure mode of brittle geomaterials. Nevertheless, the stage-dependent regulatory mechanism of
σ2 across different stress regimes remains insufficiently established, particularly under physical biaxial loading conditions that directly capture excavation-induced stress redistribution. To address this gap, comprehensive biaxial compression tests covering
σ2 levels from 0 to 36 MPa were conducted on sandstone specimens using a self-developed biaxial static–dynamic loading system. Acoustic emission (AE) monitoring and three-dimensional digital image correlation (3D-DIC) techniques were simultaneously employed to capture multiscale responses ranging from internal microcracking to macroscopic failure. The mechanical behavior, AE multifractal spectrum characteristics, RA (Rise time/amplitude)–AF (Average frequency)-based crack-type discrimination, and evolution of DIC-derived apparent strain-dominant zones were integrated to systematically quantify the influence of
σ2 on the progressive failure process. The results reveal a pronounced stage-dependent
σ2 effect, with approximately 20 MPa identified as the critical transitional stress level at which the fracture mechanism undergoes a fundamental shift. In the low
σ2 regime of 4–16 MPa, sandstone exhibits compaction-enhanced strengthening, simple and localized crack propagation, and a predominant shear fracture mode, which is consistent with a structurally stable microcracking process. However, when
σ2 reaches 20 MPa, multiple indicators—including the abrupt increase in the peak strength deviation, marked widening of AE multifractal spectra, and reversal of RA–AF crack-type proportions—show synchronous transitions. At this stage, tensile cracks exceed shear cracks for the first time, indicating a shift from a shear-dominated failure regime to a tensile–shear interactive fracture mechanism. This transition is corroborated by the DIC strain-field evolution, which shows that the localized shear-dominant strain band observed at low
σ2 evolves into a planar tensile–shear composite strain-dominant region at 20 MPa. As
σ2 increases further to 24–36 MPa, the sandstone exhibits a more complex mixed cracking pattern, characterized by the coordinated propagation of tensile and shear fractures, as well as the formation of large-scale tensile–shear conjugate structures. Therefore, the high
σ2 regime can be considered a mechanically enhanced but structurally unstable failure stage. Together, the consistent transitions observed across mechanical curves, AE multifractal indicators, crack-type discrimination, and strain-field evolution strongly support the identification of 20 MPa as the stage-dependent turning point governing the
σ2 effect. Overall, this study provides experimentally validated insights into the transitional role of the intermediate principal stress in controlling the multiscale fracture evolution of sandstone. These findings contribute to a deeper understanding of the stage-dependent failure mechanisms of brittle rocks under non-hydrostatic confinement and offer practical implications for evaluating the stability and failure risks of rock masses subjected to complex in situ stress conditions.