Sciences in Cold and Arid Regions ›› 2019, Vol. 11 ›› Issue (2): 159-172.doi: 10.3724/SP.J.1226.2019.00159.

Previous Articles    

Effects of freeze−thaw cycle and dry−wet alternation on slope stability

YaLing Chou1(),LiYuan Sun1,BaoAn Li2,XiaoLi Wang2   

  1. 1. School of Civil Engineering, Lanzhou University of Technology, Lanzhou, Gansu 730000, China
    2. Jiangsu JiaoTong Traffic Design Research Institute Co., Ltd.,Huai'an, Jiangsu 223002, China
  • Received:2018-07-30 Accepted:2019-01-02 Online:2019-04-01 Published:2019-04-29
  • Contact: YaLing Chou E-mail:chouyaling@lzb.ac.cn
  • About author:YaLing Chou, School of Civil Engineering, Lanzhou University of Technology, 287 Langongping Road, Qilihe District, Lanzhou, Gansu 730000, China. E-mail: chouyaling@lzb.ac.cn

Abstract:

The typical loess on high slopes along the BaoLan High-speed Rail, China, was selected as the research object. The influence of the freeze?thaw cycle and dry?wet alternation on the shear-strength parameters of the unsaturated loess was investigated by laboratory experimental methods. Moreover, the temperature field, seepage field, and stability of slopes with different gradients were simulated under the effect of the freeze?thaw cycle and dry?wet alternation by using the geotechnical analysis software Geo-Studio. The research results showed (1) when the freeze?thaw cycle was repeated on the slope, with the frozen depth increasing, the melted depth did the same; besides, the closed loop of isotherms formed on the slope; (2) under the action of dry?wet circulation, the negative pore-water pressure and volumetric water content showed an upward tendency. However, owing to the different slope gradients, rainfall infiltration was not the same. As time went by, the differences of the negative pore-water pressure and volumetric water content between the slopes of different gradients continued to increase; (3) with the freeze?thaw cycle and dry?wet alternation increasing, the slope-safety factor decreased. Especially in the early period, the slope-safety factor changed remarkably. For slopes undergoing freeze?thaw action, the slope-safety factor was negatively correlated with the gradient. However, with regard to slopes undergoing dry?wet alternation, the result became more complex because the slope-safety factor was related to both seepage strength and slope grade. Accordingly, further research is needed to study the effect of seepage strength and slope grade on the stability of loess slopes.

Key words: freeze?thaw action, dry?wet alternation, temperature field, seepage field, slope stability

Table 1

Results of the shear test under different numbers of cycles (ρ d=1.62 g/cm3, ω=16 % )"

Cycle number(times) Shear strength at different vertical pressures (kPa)

Cohesion force

(kPa)

Internal friction angle (°)
100 200 300 400
Freeze?thaw cycles 0 108.720 148.584 202.944 279.048 43.488 29.479
1 77.916 173.952 197.508 262.740 33.522 30.028
3 81.540 148.584 184.824 262.740 24.462 30.105
5 83.352 132.276 217.440 255.492 21.744 31.031
Dry?wet cycles 0 108.720 148.584 202.944 279.048 43.488 29.479
1 86.976 112.344 206.568 224.688 30.804 26.903
3 86.976 94.224 157.644 228.312 19.932 25.985
5 79.728 110.532 155.832 230.124 19.932 26.404

Figure 1

Change of cohesion under different numbers of cycles"

Figure 2

Change of internal friction angle under different numbers of cycles"

Figure 3

The force of the soil"

Figure 4

Slope grid division"

Figure 5

Malan thermal conductivity and unfrozen-water content/temperature chart: (a) thermal conductivity vs. temperature; and (b) unfrozen-water content vs. temperature"

Figure 6

Lishi thermal conductivity and unfrozen-water content/temperature chart: (a) thermal conductivity vs. temperature; and (b) unfrozen-water content vs. temperature"

Figure 7

Malan soil-water characteristics and permeability-function curve: (a) soil-water characteristics curve; and (b) permeability-function curve"

Figure 8

Lishi soil-water characteristics and permeability-function curve: (a) soil-water characteristics curve; and (b) permeability-function curve"

Table 2

Real-time monitoring temperature on December 2, 2016"

Time Temperature Time Temperature
00:00 ?9 °C 12:00 3 °C
02:00 ?8 °C 14:00 5 °C
04:00 ?7°C 16:00 3 °C
06:00 ?6 °C 18:00 0 °C
08:00 ?3 °C 20:00 ?6 °C
10:00 1 °C 22:00 ?7 °C

Table 3

Lanzhou annual climate profile (1971?2000 average)"

Month Diurnal minimum temperature (°C) Daily mean temperature (°C) Monthly precipitation (mm)
1 ?10.2 ?5.3 1.4
2 ?6.0 ?1.0 2.6
3 ?0.2 5.4 9.2
4 6.0 12.1 14.7
5 10.7 17.0 33.2
6 14.2 20.4 44.0
7 16.6 22.4 67.0
8 15.6 21.1 73.2
9 11.4 16.3 40.8
10 2.9 9.8 21.3
11 ?2.2 2.5 2.8
12 ?8.4 ?3.9 0.9

Table 4

Rainfall intensity at different slopes"

Rainfall intensity (mm/d) 60.9° rainfall intensity (m/h) 51.3° rainfall intensity (m/h) 45.0° rainfall intensity (m/h)
20 0.00040 0.00052 0.00060

Figure 9

Potential evaporation function (GEO-SLOPE International Ltd., 2011)"

Table 5

Overview of potential evaporation on slopes"

Condition Evaporation
Potential evaporation strength (m/h) 0.00011
Duration (h) 12
Total potential evaporation (m) 0.00132

Figure 10

Temperature field distribution"

Figure 11

Temperature field distribution of a freezing and thawing slope: (a) temperature field distribution of one freeze; and (b) temperature field distribution of one thaw"

Figure 12

Temperature field distribution of a freezing and thawing slope: (a) temperature field distribution of 3 freezes; and (b) temperature field distribution of 3 thaws"

Figure 13

Temperature field distribution of a freezing and thawing slope: (a) temperature field distribution of 5 freezes; and (b) temperature field distribution of 5 thaws"

Figure 14

Schematic diagram of the slope"

Figure 15

The negative pore-water pressure and volume moisture content at point A vary with time: (a) variation of negative pore-water pressure at point A; and (b) volume moisture change at point A"

Figure 16

The negative pore-water pressure and volume moisture content at point B vary with time: (a) variation of negative pore-water pressure at point B; and (b) volume moisture change at point B"

Figure 17

The negative pore-water pressure and volume moisture content at point C vary with time: (a) variation of negative pore-water pressure at point C; and (b) volume moisture change at point C"

Figure 18

Law of slope-safety factor over time"

Figure 19

Change of slope safety factor with freeze?thaw cycles"

Figure 20

Change of slope safety factor with freeze?thaw cycles"

Chen SY, 1997. Analysis method of slope stability considering infiltration and evaporation effect. Rock and Soil Mechanics, 2: 8−12. DOI: 10.16285/j.rsm.1997.02.002.(in Chinese)
doi: 10.16285/j.rsm.1997.02.002.(in Chinese)
Chang D , Liu JK , Li X , et al . , 2014. Experimental study on the influence of freeze—thaw cycle on the mechanical properties of Qinghai-Tibet sand. Chinese Journal of Geotechnical Engineering, 33(7):1496−1502. DOI:10.13722/j.cnki.jrme.2014.07.023.(in Chinese)
doi: 10.13722/j.cnki.jrme.2014.07.023.(in Chinese)
Chang SP , Zhang SM , 2007. Engineering Geological Handbook, Beijing: China Architecture & Building Press.
GEO-SLOPE International Ltd., 2011. Non-saturated Soil Seepage Analysis Software SEEP/W User Guid. Beijing: Metallurgical Industry Press.
Huo LX , 2008. Climate change and its hydrological response in northwest China in recent 50a. Ph.D. Thesis, Lanzhou University, pp. 136.
Jiang CY , 2013. Study on the influence of the change of shear strength characteristic parameters on the slope deformation of the fine soil slope before and after the freeze—thaw cycle. M.S. Thesis, Xinjiang Agricultural University, pp. 58.
Li H , Yu Ling , 2011. Study on stability change of subgrade slope under freezing-thawing cycle. Subgrade engineering, (5): 26−28. DOI: 10.3969/j.issn.1003-8825.2011.05.009.(in Chinese)
doi: 10.3969/j.issn.1003-8825.2011.05.009.(in Chinese)
Liu XX , 2013. Analysis of slope stability in seasonal frozen soil area. M.S. Thesis, Chongqing Jiaotong University, pp. 83.
Ni WK , Shi HQ , 2014. Influence of freezing-thawing cycles on micro-structure and shear strength of loess. Journal of Glaciology and Geocryology, 36(4): 922−927. DOI:10.7522/j.issn.1000-0240.2014.0111.
doi: 10.7522/j.issn.1000-0240.2014.0111
Shi HH , Wang DC , 2004. Effect of precipitation infiltration on stability of unsaturated soil slopes. West-china Exploration Engineering, 16(9): 36−39. DOI:10.3969/j.issn.1004-5716.2004.09.017.(in Chinese)
doi: 10.3969/j.issn.1004-5716.2004.09.017.(in Chinese)
Wan Y , Xue Q , Wu Y , Zhao L , 2015. Mechanical properties and micromechanisms of compacted clay during drying-wetting cycles. Rock and Soil Mechanics, 36(10): 2815−2824. DOI:10.16285/j.ism.2015.10.010.
doi: 10.16285/j.ism.2015.10.010
Wang FH , Li JC , Tian WP , 2009. Experiment on rainfall infiltration law of loess slope. Journal of Chang'an University (Natural Science Edition), (04): 20−24.DOI:10.19721/j.cnki.1671-8879.2009.04.005.(in Chinese)
doi: 10.19721/j.cnki.1671-8879.2009.04.005.(in Chinese)
Wang C , 2014. Study on mechanism of frost-thaw collapse of Hada Railway slope in seasonal frozen area. M.S. Thesis, Harbin Institute of Technology, pp. 74.
Wang TX , Liu ZC , Lu J , 2007.Experimental study on thermal conductivity and specific heat capacity of loess. Rock and Soil Mechanics, 28(4): 655−658. DOI: 10.16285/j.rsm. 2007.04.004.(in Chinese)
doi: 10.16285/j.rsm. 2007.04.004.(in Chinese)
Xiao DH , Feng WJ , Zhang Z , et al . , 2014. Research on the Lanzhou loess's permeabilities changing with freezing-thawing cycle. Journal of Glaciology and Geocryology, 36(5): 1192−1198. DOI:10.7522/j.issn.1000-0240.2014.0109
doi: 10.7522/j.issn.1000-0240.2014.0109
Xu H , Zhu YW , Cai YQ , et al . , 2005. Stability analysis of unsaturated soil slopes under rainfall infiltration. Rock and Soil Mechanics, 26(12):1957−1962. DOI:10.16285/j.rsm. 2005.12.020.
doi: 10.16285/j.rsm. 2005.12.020
Zhou H , Zhang Z , Feng WJ , et al . , 2014. Determination of long-term strength of frozen loess after numerous freeze—thaw cycles. Sciences in Cold and Arid Regions,6(5): 0494−0498. DOI: 10.3724/SP.J.1226.2014.00494.
doi: 10.3724/SP.J.1226.2014.00494
Zhang Z , V.Pendin Vadim , Feng WJ , et al . , 2015.The influence of freeze—thaw cycles on the granulometric composition of Moscow morainic clay. Sciences in Cold and Arid Regions,7(3): 0199−0205. DOI: 10.3724/SP.J.1226. 2015. 00199.
doi: 10.3724/SP.J.1226. 2015. 00199
Zhou J , Xu HZ , Hu WJ , 2013. Impact of wetting-drying cycle effects on stability of expansive soil slopes. Chinese Journal of Geotechnical Engineering, 35(2): 152−156.
Zhou JW , Xu WY , Deng JY , et al . , 2008.Stability analysis of slope under the condition of rainfall infiltration. Journal of hydraulic engineering,39(9): 1066−1073. DOI: 10.1324 3/j.cnki.slxb.2008.09.013.(in Chinese)
doi: 10.1324 3/j.cnki.slxb.2008.09.013.(in Chinese)
[1] LiYan Lao, ZhiQiang Ji, LiangLiang Huang, ShangJing Li. Research on the temperature field of a partially freezing sand barrier with groundwater seepage [J]. Sciences in Cold and Arid Regions, 2017, 9(3): 280-288.
[2] QingZhi Wang, BoWen Tai, ZhenYa Liu, JianKun Liu. Study on the sunny-shady slope effect on the subgrade of a high-speed railway in a seasonal frozen region [J]. Sciences in Cold and Arid Regions, 2015, 7(5): 513-519.
[3] ZuRun Yue, BoWen Tai, TieCheng Sun. Analysis of temperature field characteristics based on subgrade site measurements of Harbin-Qiqihar High-speed Railway in a deep seasonal frozen soil region [J]. Sciences in Cold and Arid Regions, 2015, 7(5): 547-553.
[4] Xi Chen, JianKun Liu, Nan Xie, HuiJing Sun. Probabilistic analysis of embankment slope stability in frozen ground regions based on random finite element method [J]. Sciences in Cold and Arid Regions, 2015, 7(4): 354-364.
[5] QingBo Bai, Xu Li, YaHu Tian. A method used to determine the upper thermal boundary of subgrade based on boundary layer theory [J]. Sciences in Cold and Arid Regions, 2015, 7(4): 384-391.
Viewed
Full text


Abstract

Cited

  Shared   
  Discussed   
No Suggested Reading articles found!