Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw Cycles

To study the dynamic characteristics and mechanism of saturated loess after freeze-thaw cycles, a series of laboratory tests including freeze-thaw cycle tests, dynamic triaxial tests, and scanning electron microscope tests of the saturated remolded loess was conducted. The characteristics of the dyn...

Full description

Saved in:
Bibliographic Details
Main Authors: Qian Wang, Fuqiang Liu, Xiumei Zhong, Zhongnan Gao, Shouyun Liang, Yuxin Liang
Format: Article
Language:English
Published: Wiley 2021-01-01
Series:Geofluids
Online Access:http://dx.doi.org/10.1155/2021/6296578
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1832561546700521472
author Qian Wang
Fuqiang Liu
Xiumei Zhong
Zhongnan Gao
Shouyun Liang
Yuxin Liang
author_facet Qian Wang
Fuqiang Liu
Xiumei Zhong
Zhongnan Gao
Shouyun Liang
Yuxin Liang
author_sort Qian Wang
collection DOAJ
description To study the dynamic characteristics and mechanism of saturated loess after freeze-thaw cycles, a series of laboratory tests including freeze-thaw cycle tests, dynamic triaxial tests, and scanning electron microscope tests of the saturated remolded loess was conducted. The characteristics of the dynamic parameters of the saturated loess after different freeze-thaw cycles were discussed. The characteristics of the microstructure parameters changes were analyzed. The evolution process and mechanism of the microstructure of the remolded loess under freeze-thaw cycles were proposed. The results show that after different freeze-thaw cycles, the dynamic stress-dynamic strain curves of the saturated remolded loess conform to the hyperbolic model; however, the freeze-thaw cycle has a significant effect on the model parameter b. With the increase of freeze-thaw cycles, the dynamic shear modulus of saturated remolded loess first decreases and then increases, while the damping ratio is opposite. When saturated remolded loess experiences freeze-thaw cycles greater than four, its dynamic stability is better than that of saturated soil without freeze-thaw cycles. The dynamic stability reaches its peak after seven freeze-thaw cycles and is equivalent to that of saturated soil without freeze-thaw cycles after forty cycles. Combined with the results of the quantitative analysis of microstructure images, with the increase of the freeze-thaw cycles, the number of large and medium particles in the soil reduces, and the number of micros and small particles increases. The particle size tends to be uniform. The apparent porosity increases rapidly and then decreases sharply and tends to be stable after 4 freeze-thaw cycles. The pore and particle fractal dimensions continue to decrease. The probability of entropy increases first and then decreases. It is illustrated that the saturated loess has mainly experienced three steps under freeze-thaw cycles: (1) fracture and expansion of original skeleton cementation, (2) damage, crushing and aggregation of the particle, and (3) compaction and reorganization of soil structure. Besides, the saturation condition significantly accelerates the evolution process of the internal structure of the soil under freeze-thaw cycles. These lead to the strengthening effect of soil dynamic stiffness under long-term freeze-thaw cycles.
format Article
id doaj-art-153b5123f586481c81f835bd241828f5
institution Kabale University
issn 1468-8115
1468-8123
language English
publishDate 2021-01-01
publisher Wiley
record_format Article
series Geofluids
spelling doaj-art-153b5123f586481c81f835bd241828f52025-02-03T01:24:42ZengWileyGeofluids1468-81151468-81232021-01-01202110.1155/2021/62965786296578Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw CyclesQian Wang0Fuqiang Liu1Xiumei Zhong2Zhongnan Gao3Shouyun Liang4Yuxin Liang5Key Laboratory of Loess Earthquake Engineering, China Earthquake Administration & Gansu Province, 450 Donggang West Road, Lanzhou 730000, ChinaKey Laboratory of Loess Earthquake Engineering, China Earthquake Administration & Gansu Province, 450 Donggang West Road, Lanzhou 730000, ChinaKey Laboratory of Loess Earthquake Engineering, China Earthquake Administration & Gansu Province, 450 Donggang West Road, Lanzhou 730000, ChinaKey Laboratory of Loess Earthquake Engineering, China Earthquake Administration & Gansu Province, 450 Donggang West Road, Lanzhou 730000, ChinaDepartment of Civil Engineering and Mechanics, Lanzhou University, 222 Tianshui South Road, Lanzhou 730000, ChinaDepartment of Civil Engineering and Mechanics, Lanzhou University, 222 Tianshui South Road, Lanzhou 730000, ChinaTo study the dynamic characteristics and mechanism of saturated loess after freeze-thaw cycles, a series of laboratory tests including freeze-thaw cycle tests, dynamic triaxial tests, and scanning electron microscope tests of the saturated remolded loess was conducted. The characteristics of the dynamic parameters of the saturated loess after different freeze-thaw cycles were discussed. The characteristics of the microstructure parameters changes were analyzed. The evolution process and mechanism of the microstructure of the remolded loess under freeze-thaw cycles were proposed. The results show that after different freeze-thaw cycles, the dynamic stress-dynamic strain curves of the saturated remolded loess conform to the hyperbolic model; however, the freeze-thaw cycle has a significant effect on the model parameter b. With the increase of freeze-thaw cycles, the dynamic shear modulus of saturated remolded loess first decreases and then increases, while the damping ratio is opposite. When saturated remolded loess experiences freeze-thaw cycles greater than four, its dynamic stability is better than that of saturated soil without freeze-thaw cycles. The dynamic stability reaches its peak after seven freeze-thaw cycles and is equivalent to that of saturated soil without freeze-thaw cycles after forty cycles. Combined with the results of the quantitative analysis of microstructure images, with the increase of the freeze-thaw cycles, the number of large and medium particles in the soil reduces, and the number of micros and small particles increases. The particle size tends to be uniform. The apparent porosity increases rapidly and then decreases sharply and tends to be stable after 4 freeze-thaw cycles. The pore and particle fractal dimensions continue to decrease. The probability of entropy increases first and then decreases. It is illustrated that the saturated loess has mainly experienced three steps under freeze-thaw cycles: (1) fracture and expansion of original skeleton cementation, (2) damage, crushing and aggregation of the particle, and (3) compaction and reorganization of soil structure. Besides, the saturation condition significantly accelerates the evolution process of the internal structure of the soil under freeze-thaw cycles. These lead to the strengthening effect of soil dynamic stiffness under long-term freeze-thaw cycles.http://dx.doi.org/10.1155/2021/6296578
spellingShingle Qian Wang
Fuqiang Liu
Xiumei Zhong
Zhongnan Gao
Shouyun Liang
Yuxin Liang
Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw Cycles
Geofluids
title Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw Cycles
title_full Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw Cycles
title_fullStr Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw Cycles
title_full_unstemmed Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw Cycles
title_short Dynamic Characteristics and Mechanism of the Saturated Compacted Loess under Freeze-Thaw Cycles
title_sort dynamic characteristics and mechanism of the saturated compacted loess under freeze thaw cycles
url http://dx.doi.org/10.1155/2021/6296578
work_keys_str_mv AT qianwang dynamiccharacteristicsandmechanismofthesaturatedcompactedloessunderfreezethawcycles
AT fuqiangliu dynamiccharacteristicsandmechanismofthesaturatedcompactedloessunderfreezethawcycles
AT xiumeizhong dynamiccharacteristicsandmechanismofthesaturatedcompactedloessunderfreezethawcycles
AT zhongnangao dynamiccharacteristicsandmechanismofthesaturatedcompactedloessunderfreezethawcycles
AT shouyunliang dynamiccharacteristicsandmechanismofthesaturatedcompactedloessunderfreezethawcycles
AT yuxinliang dynamiccharacteristicsandmechanismofthesaturatedcompactedloessunderfreezethawcycles