Three Dimensional Numerical Simulation of Immersed Tunnel Seismic Response Based on Elastic-Plastic...
Transcript of Three Dimensional Numerical Simulation of Immersed Tunnel Seismic Response Based on Elastic-Plastic...
Three Dimensional Numerical Simulation of Immersed Tunnel
Seismic Response Based on Elastic-plastic FEM1
Jin Xianlonga, Guo Yizhib and Ding Junhongc
High Performance Computing Center, Shanghai Jiao Tong University, Shanghai, China 200030, [email protected],
Keywords: elastic-plastic; numerical simulation; immersed tunnel; seismic response;
Abstract. Using the high performance computer SGI Onyx3800, this paper introduced finite element
method in simulating the seismic response of this immersed tunnel in Shanghai. First, consisted of the
immersed tunnel, soil and river, a large three dimension solid model was constructed by CAD
software according to actual size and geologic circumstance. Second, the finite element model was
finished in the CAE software, and the number of nodes and element in final finite element model
exceeded 1.2 million and 1 million respectively. Considering the complicity and the diversity of
different parts in the model, several material models with distinctive constitution relationships were
brought in the research. Contact between two parts also was considered in the research. Such contact
regions exist between soil and tunnels segment, GINA rubber gasket and tunnels segment, and
between vibration isolation rubber cushions and shear key. All these contact style were treated as
surface-to-surface style, and penalty function method was used to solve such problems. The ultimate
calculation adopted explicit dynamic algorithm and parallel domain decomposition method. The
result reveals the weak joints in this immersed tunnel under Tangshan seismic waves. It could also
provide data and references for the aseismatic design of immersed tunnel and its flexible joints.
Introduction
Ever-increasing populations of Shanghai, density of transportation and need for storage capacity have
led, inevitably, to an increased use of underground facilities. The second biggest immersed tunnel in
the world has been opened to traffic in Shanghai. Worldwide experience indicates that underground
facilities are economically effective in the framework of national and municipal economics [1].
However, because the East China including Shanghai is adjacent to the Circum- Pacific region and the
local sedimentary soil affects greatly on the seismic response of soil layers, it is necessary to study the
earthquake-resistant ability of the immersed tunnel under the Huangpu River.
Two methods are often used to analyze the dynamic response of the immersed tunnel. One method
is multi-mass-spring system method, which divides the soil into several strips and each strip serves as
a mass-spring system. The tunnel is treated as beams connected by linear springs in longitudinal and
lateral directions. Many immersed tunnel in Japan and the Pearl River tunnel in Guangzhou of China
were analyzed all using this method [2,3]. Another method is the finite element method. Limited to
the need of large memory capacity and considerable computing time, this method has not been widely
used until recently. Based on high performance computer, this paper introduced finite element method
in simulating the seismic response of this immersed tunnel in Shanghai.
Finite Element Model
Consisted of the immersed tunnel, soil and river, a large three dimension solid model is constructed
by CAD software according to actual size and geologic circumstance. To decrease the effect of
boundary conditions farthest, the whole size of this soil is determined to be 1670m×1110m×280m.
1 This project is supported by National Natural Science Foundation of China (No. 62073048).
Key Engineering Materials Vols. 274-276 (2004) pp 661-666Online available since 2004/Oct/15 at www.scientific.net© (2004) Trans Tech Publications, Switzerlanddoi:10.4028/www.scientific.net/KEM.274-276.661
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Then, the finite element model is finished in the CAE software. For the immersed tunnel segment,
GINA rubber and vibration isolation rubber, the 8-nodes solid element is used, while 4-nodes solid
element is adopted for the soil (Fig.1, Fig.2). At last, the number of nodes and element in whole finite
element model exceeds 1.2 million and 1 million respectively. Due to the fine finite element grid, the
results precision is guaranteed.
Fig.1 Finite element model of the soil Fig.2 Finite element model of immersed tunnel
In Fig. 2, Ei expressed tunnel segment i, and Ji expressed flexible joint i. When establishing the
finite element model, contact and material nonlinearity are considered in this paper.
Contact. Contact is dynamic ineraction between different parts. Such dynamic interaction exists
between the soil and immersed tunnel, GINA rubber gasket and tunnel segment, and between
vibration isolation rubber cushions and shear key (Fig.3). From a finite element point of view, the
contact entities, i.e. nodes and elements in contact, must be accurately detected. LS-DYNA has a very
efficient contact search algorithm. For simplicity, the bodies in contact are decomposed in two parts:
the slave and the master, and it is assumed that slaves entities must not go through master surfaces, i.e.
slaves nodes must not penetrate master segments, where a segment is a shell surface or a side-surface
of a volume element. The slave body usually corresponds to the finest mesh body or the softest
material body. Here, the tunnel segment is slave body, and the soil is master body. All these contact
style were treated as automic surface-to-surface style. In order to compute the contact forces, i.e. the
forces resulting from impenetrability assumption, a mathematical method is used: the penalty
function method. It consists in introducing fictitious springs between contact entities. The main point
of this method is the choice of the spring stiffness, which drives the strength of the contact
phenomenon. LS-DYNA uses special formulas to establish contact stiffness that is a function of the
geometric and material features of contact entities.
Fig.3 Contact entities in immersed tunnel joints Fig.4 Description of yield surface
Material Nonlinearity. Considering the complicity and the diversity of different parts in the
model, several material models with distinctive constitution relationships are brought in the research.
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The Drucker-Prager material model is used for the soil (Fig.4), and its yield criteria expression is:
( ) 021'
21 =−+= kJJF α . (1)
where, 1J is the first invariant of stress tensor, and '
2J is the second invariant of stress deviator. The
expressions for α and k are:
)sin3(3
sin2
φ
φα
±= . (2)
)sin3(3
cos6
φ
φ
±=
ck . (3)
The flexible joints comprised Mooney-Rivlin rubber model for GINA rubber gasket and vibration
isolation rubber cushions [4]. Its strain energy density function is defined as:
( ) ( )33 201110 −+−= ICICW . (4)
where, C10 and C01 are material constants, and can be gained from experiments. I1 and I2 are invariants
of right Cauchy-Green Tensor C.
Elastic-Plastic model for the concrete tunnel, the horizontal and vertical shear key, and the spring
model for pulling rope. The main parameters for those material models such as Mooney-Rivlin rubber
model were directly derived from experiment results. The following tables list all material parameters
for immersed tunnel.
Material type Mass density (g/cm3 ) Poisson’s ratio Elastic modulus (GPa)
Concrete tunnels segment 2.50 0.167 31.5
GINA rubber gasket 1.14 0.499 --------
vibration isolation rubber 1.14 0.499 --------
Steel shear key 7.85 0.26 201
Tab.1 The material parameters of the concrete, GINA rubber gasket and vibration isolation rubber
Layer number Shear modulus
(MPa)
Poisson’s
modulus
Mass density
(g/cm3)
Cohension
(c/KPa)
Angle of internal
friction
1 10.00 0.30 1.70 22.3 22.02
2 14.35 0.40 1.92 17 21
3 14.35 0.35 1.86 4 25.4
4 30.28 0.45 1.74 13 14.2
5 61.45 0.35 1.86 4 20.7
6 38.59 0.45 1.72 10.5 7.1
7 58.74 0.40 1.77 11.0 8.8
8 77.82 0.35 1.85 4 23.3
9 80.06 0.47 1.99 27 14.1
10 83.13 0.47 2.00 25 15.5
11 115.00 0.36 1.92 8.5 21.4
12 92.75 0.47 1.79 14 14
Tab.2 The material parameters of the soil (partially)
Algorithms
Introducing three-dimensional and nonlinear modeling method, the number of nodes and elements in
whole finite element model exceeds 1.2 million and 1 million respectively. Thus, the immersed tunnel
seismic response analysis can be considered as the transient response computing of a grand scale and
nonlinear system. However, there are some difficulties: it needs great capacity data exchange and
storage for the transient response computing of a grand scale and nonlinear system. Consequently the
serial algorithm and software used in earthquake safety evaluation cannot complete this task. In
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addition, contact detection and computation require rather complex procedures and make up for a lot
of CPU time.
To solve the difficulties above, explicit algorithm, parallel domain decomposition method and
high performance computer are used in this analysis.
Explicit Algorithm. Under seismic loads, the dynamic equation of three-dimensional finite
element system can be defined as:
)()()()( tPtKxtxCtxM =++ &&& . (5)
where, xxx ,, &&& is nodes acceleration, velocity and displacement vector respectively. ),( txMM = is
mass matrix, ),( txKK = is stiffness matrix, and ),,( txxCC &= is damping matrix. P is the exterior
loads of the whole system.
The central difference method are adopted to solve Eq.5:
2)()()()( 21212121 nnnnn txtttxtx &&&&−+−+ ∆+∆+= . (6)
)()()( 21211 +++ ∆+= nnnn txttxtx & . (7)
in Eq.6 and Eq.7, )( 21+ntx& is nodes velocity at 21+nt , and )( 1+ntx is nodes coordinate at 1+nt .
Time Step Control: during the solution we loop through the elements to update the stresses and the
right hand side force vector. We also determine a new time step size by taking the minimum value
over all elements.
{ }N
nttttt ∆⋅⋅⋅∆∆∆⋅=∆ + ,,,,min 321
1 α . (8)
where N is the number of elements. For stability reasons the scale factor α is typically set to a value
of 0.9 (default) or some smaller value.
When establishing the finite element model, solid elements are used in this paper. A critical time
step size, et∆ , is computed from:
( )( )( )2122CPPLt ee ++=∆ . (9)
where P is a function of the bulk viscosity coefficients, Le is a characteristic length.
Hourglass Control: explicit dynamic algorithm usually adopts one-point integration. The biggest
disadvantage to one-point integration is the need to control the zero energy modes which arise, called
hourglassing modes. Undesirable hourglass modes tend to have periods that are typically much
shorter than the periods of the structural response, and they are often observed to be oscillatory.
In order to control the purely numerical deformations, hourglass resisting forces are added for
cases when they are excited. Then, in the mechanical energy balance, it appears an hourglass energy
that is linked to the hourglass resisting forces against formation of hourglass modes.
Parallel Domain Decomposition Method. In this analysis, the parallel algorithm uses the domain
decomposition technique; for example, the mesh of a model is partitioned into subdomains and, in
most cases, each domain is assigned to one processor. Processors exchange boundary data by using
explicit communication tools, specifically, MPI (message passing interface).
Recursive Coordinate Bisection (RCB) Method: RCB is attractive as a dynamic load-balancing
algorithm because it implicitly produces incremental partitions. In RCB, the computational domain is
first divided into two regions by a cutting plane orthogonal to one of the coordinate axes so that half
the workload is in each of the sub-regions. The splitting direction is determined by computing in
which coordinate direction the set of objects is most elongated, based upon the geometric locations of
the objects. The sub-regions are then further divided by recursive application of the same splitting
algorithm until the number of sub-regions equals the number of processors. Although this algorithm
was first devised to cut into a number of sets which is a power of two, the set sizes in a particular cut
needn't be equal. By adjusting the partition sizes appropriately, any number of equally-sized sets can
be created. If the parallel machine has processors with different speeds, sets with nonuniform sizes
can also be easily generated.
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Fig.5 Three-dimensional model partitioning description of the immersed tunnel
Because too much contact exits in 8 flexible joints in the immersed tunnel, every sub-region
includes a flexible joint in order to achieve load balance in this partition (Fig.5).
Results
A high performance computer SGI Onyx3800 (Tab.3) completed the final calculation.
Number of CPUs Clock frequency (MHz) Memory (GB) Hard disk (TB) Perk performance (GFLOPS)
64 500 32 4.3 64
Tab.3 The technical parameters of SGI Onyx3800
Fig.6 Tangshan seismic acceleration Fig.7 The maximal relative displacement of all joints
Tangshan seismic acceleration recorded in Beijing Restaurant in 1976 (Fig.6) is used in this
analysis, and the sampling interval is 0.01 second. The maximal acceleration is 65.9 cm/s2. According
to the field safety requirement of the immersed tunnel in Shanghai, the amplitude modulation is
applied to Tangshan seismic acceleration and its maximal acceleration changes to be 100 cm/s2.
Because the vibration for underground structures is affected greatly by the excited direction of seismic
wave, three cases are considered in results analysis: seismic wave excites in X-axis direction, Y-axis
direction and Z-axis direction (in Fig.1).
The results reveal the weak joints in this immersed tunnel form Fig.7, which are J2 and J3. The
reason is that the second tunnel segment goes beyond the riverbed and it has less covering soil. Thus,
the second tunnel segment has less restriction under seismic acceleration, and the maximal relative
displacement comes into being at J2 and J3.
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(a) Interaction between tunnels and the soil (b) Displacement between two tunnels segments
Fig.8 The strain nephogram of immersed tunnel under Tangshan seismic wave
Fig.8 is about the displacement nephogram of this immersed tunnel when Tangshan seismic wave
excites in X-axis direction.
Conclusion
It is insured that the harmonious units are used in this analysis when defining material parameters,
because wrong units would affect the response and contact stiffness of the materials. The material
data in finite element model should be precise, and the reason is that the precision of most nonlinear
dynamic problems depends on the quality of material data. The initial contact between two contact
entities is not permitted, and there is no overlap in contact areas. The repetitive contact should not be
defined between two same parts.
According to the results, the deformation style and the deformation zones show the earthquake-
resistant ability of this immersed tunnel and the joints that need more attention in the future. It could
also provide data and references for the aseismatic design of immersed tunnel.
References
[1] F. Kirzhner and G. Rosenhouse: Numerical Analysis of Tunnel Dynamic Response to Earth
Motions. Tunnelling and Underground Space Technology, Vol. 15, No. 3 (2000), p.249
[2] Kiyomiya O.: Earthquake-resistant Design Features of Immersed Tunnels in Japan. Tunnelling
and Underground Space Technology, Vol. 20, No. 4 (1995), p.463
[3] Yan Songhong, Gao Bo and Pan Changshi: Dynamic Property Analysis on Joint for Submerged
Tunnel Under Earthquake. Chinese Journal of Rock Mechanics and Engineering, Vol. 22, No. 2
(2003), p.286
[4] Wei Yintao, Yang Tingqing and Du Xingwen: On the Large Deformation on Rubber-like
Materials: Constitutive Laws and Finite Element Method. ACTA MECHANICA SOLIDA SINICA,
Vol. 20, No. 4 (1999), p.281
666 Advances in Engineering Plasticity and Its Applications
Advances in Engineering Plasticity and Its Applications 10.4028/www.scientific.net/KEM.274-276 Three Dimensional Numerical Simulation of Immersed Tunnel Seismic Response Based on Elastic-
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DOI References
[2] Kiyomiya O.: Earthquake-resistant Design Features of Immersed Tunnels in Japan. Tunnelling nd
Underground Space Technology, Vol. 20, No. 4 (1995), p.463
doi:10.1016/0886-7798(95)00033-U