bursi o.s., ceravolo r., di sarno l., erdik m., … et al...assessment of the seismic vulnerability...
TRANSCRIPT
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Bursi O.S., Ceravolo R., Di Sarno L., Erdik M., Paolacci F., Sartori M., Pegon P.
SERIES Concluding Workshop - Joint with US-NEES “Earthquake
Engineering Research Infrastructures”
JRC-Ispra, May 28-30, 2013
In memory of Prof. Roy Severn
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OUTLINE
Description of the TA research project RETRO
PsD test design
Test rig configuration
Numerical Models of the bridge
Selection of input signals
Integration scheme for PsD test
Test sequence
Preliminary numerical and experimental investigation
on the seismic response of the non-isolated bridge
Design of deck seismic isolation
Design method for FP bearings
Modeling and numerical results
Conclusions
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Assessment of the seismic vulnerability of an old r.c
viaduct with frame piers and study of the effectiveness
of different isolation systems through pseudodynamic
test on a large scale model
TA Research projet: RETRO
• University Roma Tre (coordinator: Fabrizio Paolacci)
• University of Patras
• University of Naples and Sannio
• Politecnico di Torino
• Univertsity of Bogazici
• ALGA Spa Milan
Participants
F. Paolacci, R. Giannini, A. Mohamad, S. Alessadri, N. Makris, L. Di
Sarno, G. Della Corte, R. Derisi, R. Ceravolo, Luca Zanotti Fragonara, M.
Erdik, C. Yenidogan, A. Marioni, M. Sartori
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Case Study
The case study is an old r.c.
viaduct (Rio Torto) placed along
the Firenze-Bologna Highway
between Roncobilaccio and Pian
del Voglio, and was built at the end
of the 50’s
It is characterized by:
• Thirteen-span (33 m) bays deck
with two independent roadways
sustained by 12 couples of piers
• Frame piers with height variable
between 14 and 50 m
• Ductile plain steel bars
Rio-Torto Viaduct
Gerber Saddles
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Case Study Gerber Saddles
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PsD test design: Test rig configuration
• Pier 9
– Height 10.3 m
– Hollow columns 64 cm
– Top beam 3.16 x 0.64 m
– Two middle beams
• Pier 11
– Height 5.8 m
– Solid columns 48 cm
– Top beam 3.0 x 0.48 m
– One middle beams
Non isolated case
SCALE 1:2.5
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PsD test design: Test rig configuration
Non isolated case
18 Actuators will be used for the test!!!
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PsD test design: Test rig configuration
Non isolated case: scale reduction
This is a well known problem that can be easily solved using dimensional analysis.
A scale factor 1:2.5 has been assumed in order to reduce lengths (Geometry and
displacements) at a level compatible with the requirements of the experimental
setup, especially in terms of maximum capacity of the actuators (Forces). Thus
the only reduction factors to be selected are those of length and forces. The other
can be evaluated by a dimensional analysis.
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PsD test design: Test rig configuration
Non isolated case: scale reduction
The correct flexural strength of columns and transverse beams is realized with a
rigorous respect of the geometrical scaling of the prototypes, including the
reinforcement diameters and their position.
In particular for the columns of both #pier 9 and #11 plain steel rebars with
diameter of 8 and 10 mm has been used for respecting the similitude
requirements, given that the original diameters are 24 and 20 mm. Therefore only
a little approximation has been adopted for the 24 mm diameter.
About Shear strength of pier #9 and #11, because the high strength of columns
the problem is related only to transverse beams. In this case, because the full scale
diameter of the stirrups is 8 mm with maximum spacing of 20 mm, we decided
to adopt a scaled diameter of 3 mm with a spacing of 8 mm. Consequently,
whereas a correct scaling of the confinement effect is obtained, the shear strength
is a little bit underestimated, even if it is considered acceptable.
More delicate is the scaling effect on concrete–steel bond conditions.
Forturantely, because the experimental evidence has proved that in this case the
anchorage effect of hooks prevails, the simple geometrical scaling can be
accepted
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The main advantage of this solution is
that it allows keeping the same system
for vertical load application on the
piers in both the isolated and non
isolated configurations while avoiding
any interaction between the vertical
loading system and the isolators.
The vertical load will be applied to the
isolators through a different vertical
loading system that allows to impose
the same vertical load (e.g., same
pressure) as that applied to the piers
PsD test design: Test rig configuration
FP BASE ISOLATION SYSTEM
Isolated case with FP
bearings
Substructuring
techniques
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The main advantage of this solution is
that it allows keeping the same system
for vertical load application on the
piers in both the isolated and non
isolated configurations while avoiding
any interaction between the vertical
loading system and the isolators.
The vertical load will be applied to the
isolators through a different vertical
loading system that allows to impose
the same vertical load (e.g., same
pressure) as that applied to the piers
PsD test design: Test rig configuration
FP BASE ISOLATION SYSTEM
Isolated case with FP
bearings
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PsD test design: Test rig configuration
Isolated case: scale reduction
The full scale model of Friction Pendulum isolators designed according to a
displacement-based design should have a Radius R=3000 mm and a friction
coefficient equal to 4%. The ultimate axial force if about 7500 kN, whereas the
seismic axial force is about 2800 kN.
Scale
facto
r 1:
2.5
Radius: R=3000 /2.5 = 1200 mm
Friction coefficient: =4%
kNNs 112
mm
kN.
R
Ns 9330
sN
Fu
ll S
cale
Radius: R=3000 mm
Friction coefficient: =4%
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MOCK-UPS
PsD test design: Test rig configuration
10
.3 m
5.8
m
2.6
8 m
2
.84
m
3.1
0 m
2.4
0 m
2
.40
m
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MOCK-UPS
PsD test design: Test rig configuration
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PsD test design: Numerical Models
NON LINEAR
MODELING
1) Non-linear flexural
behaviour of the element
using a fiber discretization
of the sections
2) Non-linear shear
behaviour of transverse
beams using a global
model, calibrated by using
experimental results and
analytical models [Priestly,
Vecchio and Collins]
3) Strain-penetration effect
of the reinforcing bars at
the columns-foundation
joints using the Zhao and
Shitaran model
REFINED MODEL (OpenSEES)
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PsD test design: Numerical Models
Model Reduction
1) Guyan Method has been
used to reduce the single
piers into 4-3DOFs
superelement supposing
only a trasnversal
behaviour of all piers.
2) The vertical behaviour of
columns has been taken
into account using vertical
elastic springs.
3) The non-liner behaviour
of piers has been
modeled using a Bouc-
Wen softening hysteretic
spring
SIMPLIFIED MODEL (OpenSEES): Non Isolated
Guyan method
4-3 DOFs model P-DOF
Pier #9
Pier #11
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PsD test design: Numerical Models
The reduced 3DOFs model allows to handy
accomodate the isolation elements that are
simply placed between springs and link
element
SIMPLIFIED MODEL (OpenSEES): Isolated Case
Reduced DOFs model
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PsD test design: Selection of Input
Two limit states are considered for the seismic performance assessment of the “as built” Rio-Torto bridge:
Damage Limit state (DLS) Ultimate Limit State (ULS)
Given the geographical position of the bridge and the recent
earthquake swarms occurred in the region it was assumed to use the seismic records of the 2012 Emilia (Italy) earthquakes.
The Mirandola records (MRN station) were utilized because of their seismological characteristics, i.e. PGAs and duration of the accelerograms.
The record of May 29th East-West was used for the DLS and the North-South component was used to assess the seismic performance at the ULS
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PsD test design: Selection of Input
Seismogenetic zone
0 0.5 1 1.5 2 2.5 3 3.5 40
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
T (sec)
Sa
(g
)
Life Safety
Near Collapse
Damage limit
1st period
Ground shaking Response Spectra
-200 -150 -100 -50 0 50 100 150 200 250
-250
-200
-150
-100
-50
0
50
100
911912913
914915
916
917
918
919
920
921
km
km
41.5
41.75
42
42.25
42.5
42.75
43
43.25
43.5
43.75
44
44.25
44.5
44.75
45
45.25
8.5 8.759 9.259.5 9.7510 10.2510.510.7511 11.2511.511.7512 12.2512.512.7513 13.2513.513.7514 14.2514.5
0 0.1 0.2 0.3 0.4 0.5 0.60
0.05
0.1
0.15
0.2
0.25
X: 0.1225
Y: 0.2924
PGA (g)
Pro
ba
bili
ty o
f o
ccu
rence
SLV
SLC
Seismic Hazard
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PsD test design: Selection of Input
ULS DLS
Record of the 29th May 2012 (N-S Component)
Record of the 29th May 2012 (W-E Component)
ULS
DLS
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PsD test design: Integration scheme
At ELSA they have been using the so-called Continuous PsD scheme for
many years. This scheme allows to load the experimental structure
continuously (elapse time 2ms) by performing in the same loop the time
integration of the PsD model of the structure and the digital control of the
actuators loading the structure.
By avoiding the hold period associated with standard PsD implementation,
the continuous method avoids load relaxation problems, optimizes the ratio
signal/noise associated with the experimental errors, works with a constant
time dilation and thus globally improves the quality of the results.
The test of the viaduct is substructured, in the sense that a part of the
structure is in the laboratory (experimental structure), and the other part is
modeled numerically. The substructured test will be performed using an
inter-field version (Pegon 2008, Bonelli & al. 2008) of the time partitioned
scheme proposed by (Gravouil & Combescure, 2001).
This scheme works with different time steps for the two substructures. The
PsD scheme is in fact slightly modified using additional constrain steps,
which allows introducing integration substepping with respect to the time
integration of the numerical structure for which potentially complex and
non-linear models should be operated, requiring more computational time
than the 2ms needed by the PsD scheme.
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PsD test design: Integration scheme
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PsD test design: INSTRUMENTATION
2 typologies of sensors wil be used for the acquisition of kinematic quantities
Traditional instrumentation Innovative instrumentation (photogrammetry)
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PsD test design: Test Program
Two configurations will be considered during the experimental tests: Slight damaged viaduct with FP isolators (config.1) Non-isolated viaduct (config.2)
The first configuration aims at verify the protection of the piers from developing any damage during the seismic action. The third configuration aims at inducing in the piers the damage suffered by the viaduct during a moderate earthquake. The tests will be performed in the following sequence:
Identification of the dynamic characteristics of the bridge 1 test on config.2 to induce DLS condition 2 tests on config. 1 for ULS condition 1 test on config. 2 for ULS condition
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Preliminary numerical and experimental investigation
“As built” configuration
A preliminary investigation aiming at studying the seismic
response of the piers has been carried out both numerically
and experimentally.
In particular
Modal analysis
Experimental and numerical investigation on the cyclic
behaviour of the piers
Numerical simulation of the non-linear seismic response
of the entire viaduct in «as-built» configuration
This represents a useful tool to compare the response of
the viaduct during PsD test with the simulated response
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Preliminary numerical and experimental investigation
MODAL ANALYSIS OF THE VIADUCT
2nd Mode 5th Mode
x
y
x
y
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Preliminary numerical and experimental investigation
NON-LINEAR CYCLIC BEHAVIOUR OF THE PIERS
A preliminary investigation aimed at studying the cyclic behaviour of
the piers has been carried out experimentally at University Roma Tre
One of the piers have been tested in
the Laboratory of Univ. Roma Tre on
a 1:4 scale specimen and several
phenomena, typical of old frame r.c.
structures, have been observed:
• Shear cracking in the transverse
beam
• Cracks opening at the column base
and bottom
• Some slight Buckling phenomena
of the reinforcing bars
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Preliminary numerical and experimental investigation
SEISMIC NON-LINEAR RESPONSE OF THE AS BUILT VIADUCT:
ULS CONDITIONS
The results of numerical simulation of the entire viaduct subjected to the
Emilia earthquake of 29th May 2011 (NS component) are shown.
Bas
e sh
ear
(kN
) B
ase
shea
r (k
N)
Bas
e sh
ear
(kN
)
Bas
e sh
ear
(kN
) B
ase
shea
r (k
N)
Bas
e sh
ear
(kN
)
Bas
e sh
ear
(kN
) B
ase
shea
r (k
N)
Bas
e sh
ear
(kN
)
Bas
e sh
ear
(kN
) B
ase
shea
r (k
N)
Bas
e sh
ear
(kN
)
Displacement(cm) Displacement(cm) Displacement(cm) Displacement(cm)
Displacement(cm) Displacement(cm) Displacement(cm) Displacement(cm)
Displacement(cm) Displacement(cm) Displacement(cm) Displacement(cm)
P.1 P.2 P.3 P.4
P.5 P.6 P.7 P.8
P.9 P.10 P.11 P.12 FOR
CE-
DEF
LEC
TIO
N C
YCLE
S
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Preliminary numerical and experimental investigation
SEISMIC NON-LINEAR RESPONSE OF THE AS BUILT VIADUCT:
ULS CONDITIONS
The results of numerical simulation of the entire viaduct subjected to the
Emilia earthquake of 29th May 2011 (NS component) are shown.
Mo
men
t (k
Nm
) M
om
ent
(kN
m)
Mo
men
t (k
Nm
)
Mo
men
t (k
Nm
) M
om
ent
(kN
m)
Mo
men
t (k
Nm
)
Mo
met
(kN
m)
Mo
men
t (k
Nm
) M
om
ent
(kN
m)
Mo
men
t (k
Nm
) M
om
ent
(kN
m)
Mo
men
t (k
Nm
)
Curvature (1/cm) Curvature (1/cm) Curvature (1/cm) Curvature 1/cm)
Curvature (1/cm) Curvature (1/cm) Curvature (1/cm) Curvature (1/cm)
Curvature (1/cm) Curvature (1/cm) Curvature (1/cm) Curvature (1/cm)
P.1 P.2 P.3 P.4
P.5 P.6 P.7 P.8
P.9 P.10 P.11 P.12
MO
MEN
T-C
UR
VAT
UR
E C
YCLE
S
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Preliminary numerical and experimental investigation
SEISMIC NON-LINEAR RESPONSE OF THE AS BUILT VIADUCT:
ULS CONDITIONS
The results of numerical simulation of the entire viaduct subjected to the
Emilia earthquake of 29th May 2011 (NS component) are shown.
Sh
ear
(kN
) Sh
ear
(kN
) Sh
ear
(kN
)
Sh
ear
(kN
) Sh
ear
(kN
) Sh
ear
(kN
)
Sh
ear
(kN
) Sh
ear
(kN
) Sh
ear
(kN
)
Sh
ear
(kN
) Sh
ear
(kN
) Sh
ear
(kN
)
Deformation Deformation Deformation Deformation
Deformation Deformation Deformation Deformation
Deformation Deformation Deformation Deformation
P.1 P.2 P.3 P.4
P.5 P.6 P.7 P.8
P.9 P.10 P.11 P.12 SHEA
R F
OR
CE-
DEF
OR
MAT
ION
CYC
LES
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Preliminary numerical and experimental investigation
SEISMIC NON-LINEAR RESPONSE OF THE AS BUILT VIADUCT :
ULS CONDITIONS
The following main results are expected during PsD test
A maximum of 17 cm and 15 cm of lateral displacement are expected
for pier #9 and #11 respectively
The analysis of the cyclic response shows the high plastic deformations
to which pier #9 and # 11are subjected.
A pronounced pinching effect is also present in the cyclic response of
pier #11. This is due to the effect of shear and bond slip
The expected level of crack width at the column base due to the bar
slippage is of the order of 1.5 – 2 mm, as confirmed by the numerical
model
The slippage is not enough to avoid flexural damage in the columns as
shown by Moment-Curvature cycles (max ductility =3)
The level of shear damage in the transverse beam is also high (drift
1% ) as confirmed by the hysteretic behavior shown
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Design of deck isolation systems using FP bearings
The second configuration of the viaduct during PsD tests will be the isolated one
using FP bearings with single sliding surface.
To maximize the effectiveness of the deck isolation system, the Gerber saddles
have been eliminated through a transverse pre-stressing system.
The design of the isolation system is based the assessment of the lateral-load
response of each pier previously presented
The method proposed to design FP bearing is based on the static lateral
response of the bridge neglecting the distributed mass of the piers, as
confirmed by non-linear analysis on the entire viaduct. The results from
pushover analyses provide the initial pier stiffness and the yielding strength
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Design of deck isolation systems using FP bearings
The FP isolation system has been designed according to a displacement-based
design method which is presented in detail in Della Corte et al. (2011). The method
is based on the direct displacement based procedure proposed by Priestley et al.
(2007).
According to the design method, assuming a dynamic friction coefficient equal
to 0.04 and a maximum sliding displacement equal to 0.10 m, the required
radius of curvature of the FP device is equal to 3 m.
A design deck displacement shape has been assumend in order to have a
maximum drift of 0.05% corresponding to initial yelding in the piers
The strength capacity of each pier must also be checked against the peak forces
transmitted by devices at the breakaway of the motion.
8%
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Design of deck isolation systems using FP bearings
SEISMIC NON-LINEAR RESPONSE OF THE ISOLATED VIADUCT :
DLS CONDITION
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Design of deck isolation systems using FP bearings
SEISMIC NON-LINEAR RESPONSE OF THE ISOLATED VIADUCT :
ULS CONDITION
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Design of deck isolation systems using FP bearings
SEISMIC NON-LINEAR RESPONSE OF THE ISOLATED VIADUCT :
ULS CONDITION
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CONCLUSIONS
A COMPLEX EXPERIMENTAL ACTIVITY IN GOING TO BE EXECUTED FOR THE SEISMIC ASSESSMENT OF AN OLD R.C. VIADUCT BY USING A PSD TEST CAMPAIGN
THE TECHNIQUE OF NON-LINEAR SUBSTRUCTURING WILL BE USED INCLUDING A HUGE NUMBER OF DOFs.
A LARGE SCALE TEST WILL BE EXECUTED ON TWO PIERS OF THE VIADUCT, WHICH ARE IN SCALE 1:2.5
A REFINED NON-LINEAR MODEL HAS BEEN PRELIMINARY USED TO CALIBRATE A REDUCED NON-LINEAR MODEL TO BE USED DURING THE PSD TEST
TRADITIONAL AND INNOVATIVE INSTRUMENTAIONS WILL BE USED DURING THE TESTS
TWO CONFIGURATIONS WILL BE TESTED. NON-ISOLATED AND ISOLATED A FP SYSTEM HAS BEEN DESIGN ACCORDING TO A NOVEL
DISPLACEMENT DESIGN METHOD A PRELIMINARY NUMERCIAL ANALYSIS HAS BEEN CARRIED OUT ON AS-
BUILT AND ISOLATED CONFIGURATION WITH FP BEARINGS, SHOWING A LARGE DAMGE CONDITION IN THE FIRTS CASE AND THE HIGH EFFECTIVENESS IN THE SECOND ONE.