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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 1
FINITE ELEMENT CODE FOR SOIL AND ROCK ANALYSES
Plaxis Vietnam 2008 1
f i n i t e e l e m e n t c o d e f o r s o i l a n d r o c k a n a l y s e s
C tit ti S il M d l St t l El t d Si l ti
PLAXIS SEMINARVietnam Seminar
2008
THE PLAXIS APPROACH
Constitutive Soil Models, Structural Elements and Simulation
V I S U A L I S E A N A L Y S E O P T I M I S E > T H E W A Y F O R W A R D
Dr WL CHEANG & Dr SW LEE
William W.L. CHEANG B.Eng (Hons), PG.Dip, M.Sc. Ph.D
Compiled by:
Regional Technical ManagerPlaxisAsia
Contributed
Erwin BEERNINKDennis WATERMAN
Erick SEPTANIKARonald BRINKGREVE
Siew Wei LEE
LAXIS PROFESSIONAL vers ion 8 .5 - PLAXFLOW vers ion 1 .5 - DYNAMICS module - 3-D FOUNDATION vers ion 2 .0 – 3-D TUNNEL vers ion 2 .0 – 3-D GEOTHERMIE vers ion 1 .
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 2
SOIL MODELS, STRUCTURAL ELEMENTS & BOUNDARY CONDITIONS IN PLAXIS INPUT
A. Constitutive Soil Models
1. Linear Elastic (LE)
2. Mohr‐Coulomb (MC)
3 Soft soil / creep model (SSM and SSCM)3. Soft soil / creep model (SSM and SSCM)
4. Hardening Soil model (HSM)
5. User‐defined Soil Models (USM)
B. Structural Elements
1. Geotextile element (membrane)
2. Beam (Plate) element
3. Node‐to‐node anchor3. Node to node anchor
4. Fixed end anchor
C. Recent Development with Embedded Inclusion
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f i n i t e e l e m e n t c o d e f o r s o i l a n d r o c k a n a l y s e s
A SOIL MODELSA. SOIL MODELS
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 3
MOHR-COULOMB1. First order approximation of soil
2. Linear elastic perfect plasticity
3. Five material inputs
1. Friction angle (phi)g (p )
2. Cohesion (c’)
3. Dilatancy angle (psi)
4. Elastic modulus (E)
5. Poisson’s ration (nu)
Plaxis Vietnam 2008 5
SOFT SOIL & SOFT SOIL CREEP MODEL1. Inspiration from Cam‐Clay class of model
2. Primary compression for Normally consolidated soils
3. Stress dependent stiffness
4. Distinction between primary loading and unloading‐reloading4. Distinction between primary loading and unloading reloading
5. Memory of preconsolidation stress
6. Failure behaviour=Mohr Coulomb
Plaxis Vietnam 2008 6
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 4
SOFT SOIL & SOFT SOIL CREEP MODEL
Plaxis Vietnam 2008 7
HARDENING SOIL MODEL1. Second order approximation of soil
2. Advanced model for simulating soft and stiff soils (Shanz, 1998)
3. Input parameters
Plaxis Vietnam 2008 8
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 5
HARDENING SOIL MODEL
Plaxis Vietnam 2008 9
HS-SMALL1. Hardin‐Drnevich curve
2. Parameter: Go and γ0.7
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 6
f i n i t e e l e m e n t c o d e f o r s o i l a n d r o c k a n a l y s e s
B STRUCTURAL ELEMENTSB.STRUCTURAL ELEMENTS
SOIL MODELS, STRUCTURAL ELEMENTS
A. Structural Elements
1. Geotextile element (membrane)
2. Beam (Plate) element
3 Node to node anchor3. Node‐to‐node anchor
4. Fixed end anchor
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 7
STRUCTURAL ELEMENTS IN PLAXIS1. Plates and shells
2. Anchors
3. Geogrids (geotextiles)
4. Interfaces4. Interfaces
wall strip footing tunnel
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STRUCTURAL ELEMENTS IN PLAXIS
anchored wall cofferdamgeotextile wall
strut ground anchor
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 8
PLATES AND SHELLS
1. 3 or 5 noded line elements2. 3 degrees of freedom per node3. Elastic or elastoplastic behaviour4. To model walls, floors, tunnels
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INPUT PARAMETERS FOR PLATES
1. Flexural rigidity (b=1 m)
2. Normal stiffness (b=1 m)12
3 bhEEI ⋅⋅=
( )
3. Element thickness bhEEA ⋅⋅=
EAEIhd 12==
h
b
h hb
b = 1 m in plane strainb = 1 meter in axisymmetry
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 9
PLATE WEIGHTS
1. Compensate for overlap:
2. For soil weight use:g
γunsat above phreatic level
γsat below phreatic level
realsoilconcrete dw ⋅−= )( γγ
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PLATE WEIGHTS FOR TUNNELS
d real
1. Overlap is only for half the lining thickness
rinsideroutside
lining soil
r
( ) ( )1
( )outsideinside rrr += 21
( ) ( )realsoilrealconcrete ddw 21⋅−⋅= γγ
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 10
FIXED-END ANCHORS1. To model supports, anchors and struts
1. Elasto‐plastic spring element
2. One end fixed to point in the geometry,other end is fully fixed for displacement
3. Positioning at any angle
4. Pre‐stressing option
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NODE-TO-NODE ANCHORS1. To model anchors, columns and rods
1. Elasto‐plastic spring element
2. Connects two geometry points in the geometry
i i3. Pre‐stressing option
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 11
ANCHOR MATERIAL PROPERTIES
Normal stiffness, EA (for one anchor) [kN]
Spacing, L (distance between anchors) [m]Spacing, Ls (distance between anchors) [m]
Maximum anchor force for compressionand tension, |Fmax,comp| and |Fmax,tens| [kN]
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PRE-STRESSING OF ANCHORS
1. Defined in Staged construction phase
2. Both tension (grout anchor) or compression (strut) possible(g ) p ( ) p
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 12
GEOGRIDS
1. 3 or 5 noded line element2. Linear elastic behaviour3. No flexural rigidity (EI), only normal stiffness (EA)4. Only allows for tension, not for compression5. Soil/Geogrid interaction may be modelled using
interfaces
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GROUND ANCHORS
1. Combination of node‐to‐node anchor and geogrid
2 N d d h h d (2. Node‐to‐node anchor represents anchor rod (no interaction with surrounding soil)
3. Geogrid represents grout body (full interaction with grid)
4. No interface around grout body; interface would l f l fcreate unrealistic failure surface
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 13
GROUND ANCHORS
axial forces in geotextile element
real distribution of axial forces in ground anchorInput geometry
Generated mesh
Axial forces in ground anchors
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INTERFACES1. Soil‐structure interaction
1. Wall friction
2. Slip and gapping between soil and structure
2. Soil material properties p p
1. Taken from soil using reduction factor RinterCinter = Rinter * Csoiltan(φ)inter = Rinter * tan(φ)soil
2. Individual material set for interface
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 14
INTERFACESSuggestions for Rinter:
1. Interaction sand/steel = Rinter ≈ 0.6 – 0.7
2. Interaction clay/steel = Rinter ≈ 0.5
3 Interaction sand/concrete R 1 0 0 83. Interaction sand/concrete = Rinter ≈ 1.0 – 0.8
4. Interaction clay/concrete = Rinter ≈ 1.0 – 0.7
5. Interaction soil/geogrid = Rinter≈ 1.0(interface may not be required)
6. Interaction soil/geotextile = Rinter≈ 0.9 – 0.5 (foil, textile)
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INTERFACES
1. Try to omit stress oscillations at corners of stiff structures
Inflexible corner points, causing bad
stress results
Flexible corner points with improved stress
results
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 15
f i n i t e e l e m e n t c o d e f o r s o i l a n d r o c k a n a l y s e s
C STRUCTURAL ELEMENTS (RECENT)Embedded Inclusions (Piles, Anchors and Soil Nails)
C.STRUCTURAL ELEMENTS (RECENT)
GENERAL DESCRIPTION OF EMBEDDED PILES
1. FE modeling
2. Current implementation
I3. Improvements
4. Ground anchor
5. Concluding remarks
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 16
FE MODELINGSCHEMATIZATION OF PILE-SOIL SYSTEM
Plateral
Paxial
Pile‐head
Pile behavior depends on:1 Soil type
QsQn
soil masses
Qs : mantle/skin shear forcesQn : mantle/skin normal forcesF : pile base shear forces
1. Soil type
2. Stress state
3. Pile geometry
4. Pile type (Steel, concrete, timber…etc.)
5. Installation
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Fn
FsPile‐base
Fs : pile‐base shear forcesFn : pile‐base normal forces
Plaxis Vietnam 2008
FE MODELINGVOLUME PILE APPROACH
τtτs
σr
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R dα
Plaxis Vietnam 2008
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 17
FE MODELINGEMBEDDED PILE APPROACH
pile
soil
pile
tskin
Ffoot
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Skin & Base Interaction
Skin interaction model Base/Foot interaction model
kt
s
t
Skin stiffness:ks : axial stiffnesskn&kt : lateral stiffness
kskn
ks
kt
kn
ktkb
Base stiffness:kb : base/foot stiffness
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≤≤nSkin tractions:ts = qs/length = ks (us
pile‐ussoil) tmax
tn = qn/length = kn (unpile‐un
soil)tt = qt/length = kt (ut
pile‐utsoil)
≤
kskn Base/Foot force:
0 Fb = kb (ubpile ‐ ub
soil) Fmax
Plaxis Vietnam 2008
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 18
Skin & Base InteractionLinear skin traction model & Maximum base/foot force
Bearing Capacity:
½ (Ttop+Tbot)*Lpile + Fmax
Ttop
Lpile
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Fmax
Tbot
Plaxis Vietnam 2008
Mesh‐dependent behavior
P
Bearing capacityfine meshcoarse mesh
Due to soil failure inside “pile region”
36
y
Plaxis Vietnam 2008
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 19
ImprovementsI. Objective behavior (less mesh‐dependent )
“Pile zone” is defined based on the volume of pile (=πR2*L)Any small (soil) element that falls inside pile zone will be forced to remain elastic
2 R
37
Embedded Pile Element
Plaxis Vietnam 2008
ImprovementsII. Layer‐dependent maximum (allowable) skin traction model
Maximum skin traction as function of depth will be generated automatically for different layers according to
t { avg t φ }* Rts { σhavg tan φi + ci }*2πR
with:φi interface friction angle (Rp* φsoil)ci interface cohesion (Rp* csoil)σh
avg average lateral compression at the pile(based on soil stresses around the pile)
≤
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extra control paramaters:tsmax user‐defined maximum valueΔσh user‐defined pre‐stress to include local confinement
Plaxis Vietnam 2008
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 20
ImprovementsIII. Multi‐linear curve of maximum (allowable) skin traction
Ttop
Ty1
ytop
y1
Ty3
Ty2
Ty4
y2
y3
y4
39
Ty5y5
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Improvements IV. Installation Effects
Pile centre
Pile zone
Disturbed/influenced soil region
void ratio eσ may decrease/increase
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 21
Ground anchors
A Ground anchor model consists of* anchor* grout body
B
wall
grout body
anchor
FE modeling:Anchor 2‐noded springGrout body embedded pile
(allowing sliding)
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C
Plaxis Vietnam 2008
CONCLUDING REMARKS ON EMBEDDED ELEMENTS
1. Embedded pile has been implemented in 3DF
* Bearing capacity : maximum skin traction & base/foot resistance
1 Mesh effect is handled by including elastic region inside “pile zone”1. Mesh effect is handled by including elastic region inside pile zone
2. Current version appears capable of predicting “objective” failure behavior
* layer‐dependent (maximum) skin tractions will be included
1. Future version
* multi‐linear curve of maximum skin tractions (available in 3DF V2)
* installation effects (case studies & field experience)
G d h d l b d E b dd d il h
42
1. Ground anchor model based on Embedded pile approach
Plaxis Vietnam 2008
finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 22
PILED RAFT FOUNDATION FOR A STORAGE TANK
CHARACTERISTICS
1.No. of Piles 122
2.Pile Diameter 400mm
3.Pile Lengths 5m and 8m (staggered)
4.Raft 1000mm THK
5.Raft Size
6 Tank Diameter 10m6.Tank Diameter 10m
7.TankThickness 1000mm
8.Soil Layered
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finite element for soil and rock analyses
PLAXIS SEMINAR‐ Taipei 2007 23
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finite element for soil and rock analyses
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