numerical simulation of static liquefaction in tailings pond

5
Numerical simulation of Static Liquefaction in tailings pond Yang Liu 1, a , Xuetong Zhao 1, b ,Hongxiang Yan 1, c 1 Department of Civil Engineering, University of Science and Technology Beijing, 100083, China a [email protected], b [email protected], c. [email protected] Keywords: Static Liquefaction; Numerical simulation; Tailings pond Abstract. Static liquefaction is one of the main causes of flow slide destruction in tailings pond. This paper analyzed the static liquefaction behaviors in tailings pond through the development of displacement, deformation and pore pressure ratio. Based on the simulation results, some conclusions were obtained. Fast discharge of tailings will fasten the increase of pore pressure. The dam-toe in tailings pond is very easy to be eroded, leading to introverted destruction. The liquefaction of sand layer in foundation would cause the tailings dam’s slip failure. With the arising of tailings, pore pressure increased continuously expanding to the foundation under the dam. Introduction Tailing pond plays an very crucial role in the mine production, which is the most important facility maintaining the normal production of mine. It is also an artificial debris flow sources involves much potential energy, which will lead to dam break and bring about such serious accidents as inundating the crops, channel filling, environment pollution. The destruction is much more serious than the dam break of common dam[1,2]. The instability induced by liquefaction is one of the main causes leading to the dam break. One part of sand liquefaction is caused by static loading and another part is the re-circulated liquefaction caused by dynamic loading including earthquake, explosion and mechanical vibration. There are so many researches on the re-circulated liquefaction, while only few researches focused on the static liquefaction, static liquefaction didn’t draw attention in recent decades, so the research on static liquefaction fall behind that of re-circulated liquefaction in China. Static liquefaction is the most common destruction to tailings pond, it has drawn great attention abroad, but lacking of research at home[3]. This paper adopt the Two-invariant Superior Sand Model developed by Boukpeti, then conduct a numerical simulation on tailings pond under static loading, finally analyze the static liquefaction behavior by the global stability, displacement, pore pressure and deformation[4,5]. Static liquefaction Static liquefaction can be defined as pore pressure increases in saturated sand soil under static loading decreasing the shear strength and effective stress, then sand will behave like fluid. The principle is shown in fig1, st τ is the initial stress of sand, Φ cv is the critical stress ratio. Curve 1 and curve 2 are stress paths under monotonic load and cyclic load respectively. However, the transient load produced by both of them will cause the liquefaction of sandy soil. As shown in fig1, when the stress exceeds the failure line, the shear strength will decrease sharply to the stable state corresponding to the residual strength ut s . Although different stress path of monotonic load and cyclic load, they reach the same final state. In Fig1, the response of monotonic load suggests that sand’s shear strength reaches peak under small strain and then decrease to the stable state correspond to the residual strength, during the shear process, sand always in a state of shear shrinkage, at the same time, pore pressure increase constantly and effective stress decrease, when reaches the later stage of the softening sand will deform continuously under the condition of constant shear and constant strain. Advanced Materials Research Vols. 671-674 (2013) pp 76-79 Online available since 2013/Mar/11 at www.scientific.net © (2013) Trans Tech Publications, Switzerland doi:10.4028/www.scientific.net/AMR.671-674.76 All rights reserved. No part of contents of this paper may be reproduced or transmitted in any form or by any means without the written permission of TTP, www.ttp.net. (ID: 155.223.64.100, Ege Üniversitesi, Izmir, Turkey-20/12/14,13:38:06)

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Numerical simulation of Static Liquefaction in tailings pond

Yang Liu1, a, Xuetong Zhao1, b,Hongxiang Yan1, c 1Department of Civil Engineering, University of Science and Technology Beijing, 100083, China

[email protected],

b [email protected],

[email protected]

Keywords: Static Liquefaction; Numerical simulation; Tailings pond

Abstract. Static liquefaction is one of the main causes of flow slide destruction in tailings pond. This

paper analyzed the static liquefaction behaviors in tailings pond through the development of

displacement, deformation and pore pressure ratio. Based on the simulation results, some conclusions

were obtained. Fast discharge of tailings will fasten the increase of pore pressure. The dam-toe in

tailings pond is very easy to be eroded, leading to introverted destruction. The liquefaction of sand

layer in foundation would cause the tailings dam’s slip failure. With the arising of tailings, pore

pressure increased continuously expanding to the foundation under the dam.

Introduction

Tailing pond plays an very crucial role in the mine production, which is the most important facility

maintaining the normal production of mine. It is also an artificial debris flow sources involves much

potential energy, which will lead to dam break and bring about such serious accidents as inundating

the crops, channel filling, environment pollution. The destruction is much more serious than the dam

break of common dam[1,2].

The instability induced by liquefaction is one of the main causes leading to the dam break. One part

of sand liquefaction is caused by static loading and another part is the re-circulated liquefaction

caused by dynamic loading including earthquake, explosion and mechanical vibration. There are so

many researches on the re-circulated liquefaction, while only few researches focused on the static

liquefaction, static liquefaction didn’t draw attention in recent decades, so the research on static

liquefaction fall behind that of re-circulated liquefaction in China. Static liquefaction is the most

common destruction to tailings pond, it has drawn great attention abroad, but lacking of research at

home[3].

This paper adopt the Two-invariant Superior Sand Model developed by Boukpeti, then conduct a

numerical simulation on tailings pond under static loading, finally analyze the static liquefaction

behavior by the global stability, displacement, pore pressure and deformation[4,5].

Static liquefaction

Static liquefaction can be defined as pore pressure increases in saturated sand soil under static loading

decreasing the shear strength and effective stress, then sand will behave like fluid. The principle is

shown in fig1, stτ is the initial stress of sand, Φcv is the critical stress ratio. Curve 1 and curve 2 are

stress paths under monotonic load and cyclic load respectively. However, the transient load produced

by both of them will cause the liquefaction of sandy soil. As shown in fig1, when the stress exceeds

the failure line, the shear strength will decrease sharply to the stable state corresponding to the

residual strength uts . Although different stress path of monotonic load and cyclic load, they reach the

same final state.

In Fig1, the response of monotonic load suggests that sand’s shear strength reaches peak under

small strain and then decrease to the stable state correspond to the residual strength, during the shear

process, sand always in a state of shear shrinkage, at the same time, pore pressure increase constantly

and effective stress decrease, when reaches the later stage of the softening sand will deform

continuously under the condition of constant shear and constant strain.

Advanced Materials Research Vols. 671-674 (2013) pp 76-79Online available since 2013/Mar/11 at www.scientific.net© (2013) Trans Tech Publications, Switzerlanddoi:10.4028/www.scientific.net/AMR.671-674.76

All rights reserved. No part of contents of this paper may be reproduced or transmitted in any form or by any means without the written permission of TTP,www.ttp.net. (ID: 155.223.64.100, Ege Üniversitesi, Izmir, Turkey-20/12/14,13:38:06)

Fig.1 The response of saturated loose sand of tailings under monotonic load and cyclic load

Numerical model

This paper adopt the Two-invariant Superior Sand Model developed by Boukpeti[6] which is

improved continuously, this model is an elastoplastic model with single yield surface, which consider

the basic characters of sand’s static liquefaction, and provide an good prediction ability. The

constitutive model is combined into FLAC to simulating the Canada liquefaction test(CANLEX).

The materials yield, plastic fluid, softening, and the plastic strain after yield can be analyzed precisely

by FLAC, furthermore static and dynamic analysis also behave very well. CANLEX conducts the site

full-scale test for loose saturated sand’s liquefied flow slide under fast loading. In the test ,the dam is

constructed on the processed sandy soil foundation, Original water table in the sand is 318m, the dam

consist of clay, it’s 8m high and the ratio of slop is 2.5:1. Containment dam consists of sand and is

10m high. In the test, the loose saturated sand of tailings discharges rapidly. The test model is shown

in Fig.2 and material parameter is given in table.1.

Fig.4 Canada liquefaction test’s section view

Table.1 CANLEX material physical mechanical parameter

Material Bulk modulus

(kpa)

Shear modulus

(kpa)

cohesion

(kpa)

Internal frictional

angle(°)

Hydraulic

conductivity

(m/sec)

density

(T/m3)

Clay dam

Containment dam

Sand of tailings

Sand of foundation

30000

30000

10000

2100

30000

30000

100

210

30

0

2

3

0

36

0

33

1×10-8

8×10-6

1×10-4

3.25×10-7

1.5

2.0

1.7

1.9

Numerical results

Fig.2 and Fig.3 show the changes of pore pressure and pore pressure ratio. As shown in Fig.2, the pore

pressure value of the sand layer of foundation is larger than other areas and decrease in the clay dam’s

direction, which is caused by Seepage drainage of foundation. The pore pressure of dam-toe at clay

dam’s upstream changes a lot, while that of downstream changes little. With the rising of tailings, the

pore pressure of upstream increase and seepage developed continuously, and dam-toe eroded by pore

pressure and seepage.

Advanced Materials Research Vols. 671-674 77

Pore pressure ratio is shown in Fig.3, the pore pressure ratio of top layer is larger, which suggests

that tailings water hasn’t drained by seepage and the layer contain large water. Compare the pore

pressure ratio of 4m (Fig.3 (a)) with that of 8m (Fig.3 (b)), pore pressure of inside dam toe increase

continuously with the rising of tailings, at this development, inside dam toe will liquefy and flow, and

the dam will dump inside, at the same time, pore pressure ratio of the foundation layer under dam

increases and lead to the foundation’s liquefaction.

(a) Pore pressure of 4m

(b) Pore pressure 8m

Fig.2 Pore pressure at specific depth of tailings layer

(a) Pore pressure ratio of 4m

(b) Pore pressure ratio of 4m

Fig.3 Pore pressure ratio at specific depth of tailings layer

If the depth of the tailings reaches 16m, which can be realized in the test by increasing the weight

of the material, the simulation is shown in Fig.4, pore pressure ratio of the foundation under dam arise

to very large value, the pore pressure ratio reaches 0.7 to 0.9, so the foundation has liquefied, the

maximum of displacement reaches1.83cm, which means serious deformation, move outside at

upstream and arch upward obliquely at downstream.

(a). The pore pressure of 16m

78 Construction and Urban Planning

(b). The pore pressure ratio of 16m

(c) the displacement vector of 16m

Fig.4 Simulation results of 16m

Conclusion

This paper analyzed the static liquefaction behaviors in tailings pond and some conclusions were

obtained as following:

(1) Faster the tailings is discharged, harder the pore pressure dissipates; with the arise of tailings,

the pore pressure of foundation layer increases continuously expanding to the clay dam.

(2) The dam toe at the upstream of dam behave apparent rotational trend under the pushing of

tailings and seepage. However, the dam toe at the downstream of dam arches upward.

(3)The rapid arising of tailings will cause the foundation liquefied and flow, and then the dam

breaks.

Acknowledgments

The authors appreciate the financial support of the Program for New Century Excellent Talents in

University (No. NCET-11-0579) and the Fundamental Research Funds for the Central Universities of

China.

References

[1] Xuyang Xie, Wenqi Tian, Yunhai Wang, Xingkai Zhang: Journal of Safety Science and

Technology. Vol. 02 (2009), p5. (In Chinese)

[2] Lihong Yang, Quanming Li, Quangming Cheng, Yunhai Wang: Journal of Safety Science and

Technology, Vol. 4, No. 5 (2008), p28. (In Chinese)

[3] M. Rico, G.. Benito, A. Diez-Herrero: Journal of Hazardous Materials, Vol. 154, No. 1

(2008),p79.

[4] Psarropoulos, Prodromos N, Tsompanakis, Yiannia: Canadian Geotechnical Journal, Vol. 45, No.

5 (2008), p663.

[5] Claudio di Prisco, Silvia Imposimato: International Journal of Solids and Structures, Vol. 39, No.

13 (2002), p3523.

[6] Boukpeti N, Mroz Z, Drescher A: Canadian Geotechnical Journal, Vol. 39, No. 6 (2002), p1243.

Advanced Materials Research Vols. 671-674 79

Construction and Urban Planning 10.4028/www.scientific.net/AMR.671-674 Numerical Simulation of Static Liquefaction in Tailings Pond 10.4028/www.scientific.net/AMR.671-674.76

DOI References

[3] M. Rico, G. Benito, A. Diez-Herrero: Journal of Hazardous Materials, Vol. 154, No. 1 (2008), p.79.

http://dx.doi.org/10.1016/j.jhazmat.2007.09.110 [4] Psarropoulos, Prodromos N, Tsompanakis, Yiannia: Canadian Geotechnical Journal, Vol. 45, No. 5

(2008), p.663.

http://dx.doi.org/10.1139/T08-014 [5] Claudio di Prisco, Silvia Imposimato: International Journal of Solids and Structures, Vol. 39, No. 13

(2002), p.3523.

http://dx.doi.org/10.1016/S0020-7683(02)00164-6 [6] Boukpeti N, Mroz Z, Drescher A: Canadian Geotechnical Journal, Vol. 39, No. 6 (2002), p.1243.

http://dx.doi.org/10.1139/t02-066