Rock and Soil Mechanics ›› 2023, Vol. 44 ›› Issue (1): 171-182.doi: 10.16285/j.rsm.2022.0263

• Fundamental Theroy and Experimental Research • Previous Articles     Next Articles

Uniaxial compression behavior of fissured loess disturbed by vibration load

XU Jian1, 2, ZHOU Li-yang1, HU Ke1, LI Yan-feng1, WU Zhi-peng1   

  1. 1. School of Civil Engineering, Xi’an University of Architecture and Technology, Xi’an, Shaanxi 710055, China; 2. Shaanxi Key Laboratory of Geotechnical and Underground Space Engineering, Xi’an University of Architecture and Technology, Xi’an, Shaanxi 710055, China
  • Received:2022-03-07 Accepted:2022-08-01 Online:2023-01-16 Published:2023-01-13
  • Supported by:
    This work was supported by the National Natural Science Foundation of China (51878551).

Abstract: Uniaxial compression behavior of fissured loess after vibration was investigated by small-scale shaking table and uniaxial compression test. The test results show that the failure modes of fissured loess can be classified as four types, i.e. fracture failure, slip failure, coupled slip-fracture failure and compression-shear failure. The failure modes of fissured loess in uniaxial compression test are less affected by vibration, while it mainly controlled by fissure angle. Furthermore, vibration has little influence on the type and characteristic of the stress-strain curves, which constantly presents characteristics of strain softening. It is worth noting that the curves of loess samples with fissure angle of 45° show bimodal variation, and the second peak strength is generally larger than the first counterpart. The uniaxial compressive strength (UCS) approximately decreases linearly with growing vibration amplitude and frequency. With the increase of fissure angle, the UCS exhibits "double V" changes regardless of vibration parameters. A binary medium model is finally established, and it can well predict the stress-strain behavior and UCS of fissured loess after vibration.

Key words: vibration, fissured loess, uniaxial compression, binary medium constitutive model

CLC Number: 

  • TU 444
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