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Mechanical response of shallow foundations - Some experimental/theoretical and numerical issues: monotonic loading
IntroductionProf. ing. Claudio di Prisco
2
Prof. ing. Claudio di Prisco
Experimental device
10 20 30–800
–400
0
400
800
Time (sec)
Acc
. (g
al) Max= 712 gal
20 40 60 80 100 120–600–400–200
0200400600
Time (sec)
Acc
. (g
al) Max= 608 gal
Shear stacksShear stacks
3
Prof. ing. Claudio di Prisco
Experimental evidence
4
Prof. ing. Claudio di Prisco
The elasto-perfectly plastic approach
5
Prof. ing. Claudio di Prisco
Coupled elastoplastic CONSTITUTIVE RELATIONSHIP
qqQQDQ pttt ))(,,(
dq C dQ
Defined in quasi static conditions:
THE MACRO-ELEMENT THE MACRO-ELEMENT CONCEPTCONCEPT
333231
232221
131211
CCC
CCC
CCC
C
Incremental constitutive relationship
FOUNDATION
NEAR FIELD
FAR FIELD
6
Prof. ing. Claudio di Prisco
The interaction domain for rigid footings
Interaction domain for rigid strip Interaction domain for rigid strip footings and elasto-perfectly plastic footings and elasto-perfectly plastic approachapproach
m = M/ψBVMAX,
h = H/μVMAX
ξ = V/VMAX
1. To each point belonging to the failure locus a distinct failure mechanism corresponds
2. Difficulty in defining the failure locus when loose sand strata are concerned
3. Non-associated flow rule
4. Within the failure locus the mechanical behaviour is assumed to be elastic and uncoupled
5. Extension to rectangular footings
MONOTONOUSLY INCREASING LOADING
7
Prof. ing. Claudio di Prisco
Settlements
-0.002 -0.001 0 0.001 0.002horizontal displacement (m )
-120
-80
-40
0
40
80
120
ho
rizo
nta
l lo
ad
(k
N/m
)
Cyclic Load
Centered vertical load Centered inclined load
Cyclic inclined loading
anisotropic hardening
Cremer et al, 2001
8
Prof. ing. Claudio di Prisco
Hardening
22 2
2 1 0c
M H Vf V
B V
Isotropic hardening (Nova and Montrasio, 1991)
Swipe testsButterfield and Gottardi, 2003
H
V
V
M/B
c=Vc / VMAX
Hardening parameter
9
Prof. ing. Claudio di Prisco
Inclined-eccentric loads
Nova and Montrasio, 1991
Inclined and eccentric loadingInclined and eccentric loading
10
Prof. ing. Claudio di Prisco
How can R0 be determined?
Some hints about settlement evaluation
Homogeneous stratigraphic profiles
11
Prof. ing. Claudio di Prisco
Settlement evaluation
• Irreversibility of the material mechanical response
• Non-linearity
• Dependency of stiffness on confining pressure
12
Prof. ing. Claudio di Prisco
The elastic solution
Poulos e Davis (1974)
Gibson (1973)
Winkler (1867)
Dependency of stiffness on confining pressure:
0( )E z E z
Eo/λD
1
0
0.5
r/D0 1
= 0.5
13
Prof. ing. Claudio di Prisco
Settlement evaluation
The elastic solutionThe elastic solution
21q BI
E
Linear loading distribution Strip loading distribution
Rectangular loading distribution
14
Prof. ing. Claudio di Prisco
Generalised plasticity
dq I)pl
( ( , ) ciclig
Q
15
Prof. ing. Claudio di Prisco
Numerical validation
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Prof. ing. Claudio di Prisco
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Prof. ing. Claudio di Prisco
Cyclic loads
c)
b)
a)
Loose sandLoose sand Dense sandDense sand
18
Prof. ing. Claudio di Prisco
Numerical validation
19
Prof. ing. Claudio di Prisco
Numerical results
1E-005 0.0001 0.001 0.01 0.1
rocking angle (rad)
0
0.2
0.4
0.6
0.8
1
K
/ K 0
(-)
dense sandVM A X /V = 2VM A X /V = 4VM A X /V = 6VM A X /V = 8VM A X /V = 10
1E-005 0.0001 0.001 0.01 0.1
rocking angle (rad)
0
0.2
0.4
0.6
0.8
1
K
/ K 0
(-)
medium density sandVM A X /V = 2VM A X /V = 4VM A X /V = 6VM A X /V = 8VM A X /V = 10
1E-005 0.0001 0.001 0.01
rocking angle (rad)
0
0.1
0.2
0.3
0.4
dam
pin
g (
-)
dense sandV M A X /V = 2V M A X /V = 4V M A X /V = 6V M A X /V = 8V M A X /V = 10
1E-005 0.0001 0.001 0.01
rocking angle (rad)
0
0.1
0.2
0.3
0.4
dam
pin
g (
-)
m edium density sandV M A X /V = 2V M A X /V = 4V M A X /V = 6V M A X /V = 8V M A X /V = 10
20
Prof. ing. Claudio di Prisco
Cyclic consequences of the mechanical coupling
21
Prof. ing. Claudio di Prisco
22
Prof. ing. Claudio di Prisco
23
Prof. ing. Claudio di Prisco
A dynamic/non seismic problem
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Prof. ing. Claudio di Prisco