1. 南京工程学院 建筑工程学院,江苏,南京,211167
2. 南京工程学院 电力基建设施智能建造与智慧运维江苏省高校重点实验室,江苏,南京,211167
3. 长江科学院 水利部岩土力学与工程重点实验室,湖北,武汉,430010
4. 河海大学 岩土工程科学研究所,江苏,南京,210098
网络首发:2026-03-17,
纸质出版:2026
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姜景山, 左永振, 程展林, 等. 粗粒料力学特性的应力路径大型真三轴试验研究[J]. 岩土力学, 2026,47(3).
JIANG Jing-shan, ZUO Yong-zhen, CHENG Zhan-lin, et al. Large-scale true triaxial experimental study on the stress path dependence of mechanical properties of coarse-grained material[J]. 2026, 47(3).
姜景山, 左永振, 程展林, 等. 粗粒料力学特性的应力路径大型真三轴试验研究[J]. 岩土力学, 2026,47(3). DOI: 10.16285/j.rsm.2025.0248.
JIANG Jing-shan, ZUO Yong-zhen, CHENG Zhan-lin, et al. Large-scale true triaxial experimental study on the stress path dependence of mechanical properties of coarse-grained material[J]. 2026, 47(3). DOI: 10.16285/j.rsm.2025.0248.
粗粒料的力学特性表现出显著的应力路径依赖性,然而,目前开展复杂三维应力路径的大型真三轴试验研究还相对较少。为研究应力路径对粗粒料变形和强度特性的影响,开展了等小主应力、等中主应力系数(等等)与等平均正应力、等中主应力系数(等等)两种应力路径的大型真三轴各向等压固结排水剪切试验。结果表明,应力路径对粗粒料的应力−应变关系产生显著影响,随着中主应力系数的增大,等等应力路径下应力−应变曲线逐渐升高变陡,体缩变形逐渐增大,而在等等应力路径下应力−应变曲线逐渐降低变缓,体应变先压缩后膨胀,且体应变速率和体胀变形均逐渐增大。中主应力系数从0增大至0.25时,中主应变由膨胀变形逐渐转变为压缩变形;当中主应力系数从0.25增大到1.00时,中主应变均为压缩且压缩变形逐渐增大。应力路径对粗粒料的强度也有明显影响,随着中主应力系数b的增大,等等应力路径下强度逐渐增大,而等等应力路径下强度则逐渐减小。破坏内摩擦角随中主应力系数的增大而增大,且等等应力路径的破坏内摩擦角高于等等应力路径的破坏内摩擦角,固结应力较低时破坏内摩擦角更大。中主应力系数从0增大到0.75时,破坏应力比逐渐减小且减幅递减,固结应力较低时破坏应力比更高。当中主应力系数在0.75~1.00之间变化时,破坏应力比基本保持恒定。应力路径对粗粒料三维应力状态下的变形和强度特性均有重要影响,正确认识应力路径对粗粒料力学特性的影响对于科学实施土石坝工程具有重要意义。
The mechanical characteristics of coarse-grained materials exhibits a significant dependency on the stress path
and the large-scale true triaxial tests of complex three-dimensional stress paths are rarely reported. To investigate the influence of stress paths on the deformation and strength characteristics of coarse-grained materials
large-scale true triaxial isotropic consolidation and drained shear tests were carried out under two stress paths: constant minor principal stress and intermediate principal stress coefficient (constant and )
and constant mean normal stress and intermediate principal stress coefficient (constant p and ). The results indicate that the stress path has a significant influence on the stress-strain relationship. As the intermediate principal stress coefficient b increases
the stress-strain curve under the stress path of constant and b gradually ascends and becomes steeper
and the volumetric contraction deformation gradually enlarges. However
under the stress path of constant p and
the stress-strain curve descends and becomes more gradual
and the volumetric change initially compresses and then expands
accompanied by an increase in the volumetric change rate
and the dilatancy deformation gradually increases. The intermediate principal strain undergoes a transition from dilation to compression as the intermediate principal stress coefficient
increases from 0 to 0.25. When b exceeds 0.25 and reaches 1.00
the intermediate principal strain consistently exhibits compressive behavior
and the compressive deformation gradually increases. The stress path exerts a pronounced influence on the strength of coarse-grained material. Under the constant and stress path
the strength progressively enhances with the increasing intermediate principal stress coefficient
. Conversely
a progressive diminution of strength is observed under the constant and stress path as increases. The peak internal friction angle exhibits a positive correlation with the intermediate principal stress coefficient
and the peak internal friction angle of the constant p and stress path is higher than that of the constant and stress path. Additionally
lower consolidation stresses yield greater peak internal friction angles. The failure stress ratio exhibits a monotonic decrease with diminishing decrement rates as the intermediate principal stress coefficient increases from 0 to 0.75
while lower consolidation stresses correspond to higher failure stress ratio. When the intermediate principal stress coefficient varies between 0.75 and 1.00
the failure stress ratio basically remains constant. The stress path exerts a significant influence on the deformation and strength characteristics of coarse-grained materials under three-dimensional stress states. Accurate understanding of these mechanical characteristics is crucial for scientific implementation of earth-rockfill dam engineering.
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