evaluating assumptions for seismic assessment of existing buildings
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Soil Dynamics and Earthquake Engineering 27 (2007) 223233
Evaluating assumptions for seismic assessment of existing buildings
V.G. Bardakis, S.E. Dritsos
Department of Civil Engineering, University of Patras, Patras 26500, Greece
Received 15 December 2005; received in revised form 5 July 2006; accepted 6 July 2006
Abstract
This paper evaluates the American FEMA 356 and the Greek GRECO (EC 8 based) procedural assumptions for the assessment of the
seismic capacity of existing buildings via pushover analyses. Available experimental results from a four-storeyed building are used tocompare the two different sets of assumptions. If the comparison is performed in terms of initial stiffness or plastic deformation
capacities, the different partial assumptions of the procedures lead to large discrepancies, while the opposite occurs when the comparison
is performed in terms of structural performance levels at target displacements. According to FEMA 356 assumptions, effective yield
point rigidities are approximately four times greater than those of EC 8. Both procedures predicted that the structure would behave
elastically during low-level excitation and that the structural performance level at target displacement for a high-level excitation would be
between the Immediate Occupancy and Life Safety performance levels.
r 2006 Elsevier Ltd. All rights reserved.
Keywords: RC buildings; Performance-based seismic assessment; Non-linear procedures; Pushover analysis; Effective rigidities; Plastic hinge rotations;
Chord rotations
1. Introduction
Pushover procedures, to evaluate the seismic capacity of
existing buildings, represent the current trend in structural
engineering and promise a more accurate prediction of a
structures behaviour. The American pre-standard FEMA
356 [1] and the recent draft version of Part 3 of the
European Code EC 8[2], which is founded on relevant fib
[3,4]and CEB[5]reports, adopt the above procedures but
have different partial assumptions.
The draft Greek Retrofitting Code, GRECO [6], acting
within the EC 8 framework, accepts the whole European
procedure but suggests the displacement coefficient meth-od, DCM, to determine the target displacement, while EC
8[2]proposes the N2 method[7].
The present paper aims to compare the influence of the
different assumptions of the American pre-standard and
the European Codes for the assessment of existing
buildings via pushover analyses. However, since both
FEMA 356 [1] and GRECO [6] adopt the DCM methodand since a comparison of differences due to the method
of determining the target displacement is outside the scope
of this paper, GRECO [6] has been chosen for a more
direct comparison between the American and the European
procedures.
Available experimental results from a four-storeyed
building, tested at the ELSA Laboratory [8,9], have been
used as reference data to compare the two different sets of
assumptions. Performance-based evaluations have been
made for two levels of seismic action. The first level was
considered as the serviceability earthquake (low-level
excitation) while the second level was considered as themaximum design earthquake (high-level excitation).
The results of these evaluations are used for a detailed
comparison and are divided into the following two parts.
The first part of the paper focuses on local character-
istics. Different approximations to determine the available
plastic hinge or chord rotation of RC elements at every
performance level and the effective rigidity at yielding have
been assessed.
The second part of the paper presents a comparison of
elastic periods of vibration, performance points or target
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0267-7261/$ - see front matterr 2006 Elsevier Ltd. All rights reserved.
doi:10.1016/j.soildyn.2006.07.001
Corresponding author. Tel.: +30 2610997780; fax: +30 2610996575.
E-mail addresses: [email protected], [email protected]
(S.E. Dritsos).
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displacements, plastic mechanisms, drift distributions and
locations of plastic hinges. These global characteristics,
calculated according to the two procedures (FEMA 356[1]
and GRECO [6]), are also compared with the available
experimental values.
2. Building description
A full-scale four-storeyed bare frame building model,
constructed and tested in 1992 at the ELSA Laboratory
[8,9], has been used for the analytical work of the present
study. The building was designed as a high ductility framed
structure, according to the then current drafts of EC 8 [10]
and EC 2 [11]. The materials used for the building model
were normal concrete of grade C25/30 and B500 steel
reinforcement bars and welded meshes[8,9]. The buildings
behaviour factor, q, was assumed to equal 5 [8,9]. Fig. 1
presents the plan of the building model. Dimensions in plan
were 10m 10 m, measured from the column centrelines
[8,9]. The inter-storey height of the ground floor level was
3.5 m and the other inter-storey heights were 3.0 m [8,9].
Further details concerning the construction of the building
model, the mechanical characteristics of the materials and
the amount of reinforcement can be found in the ELSA
report[9].
3. Non-linear element modelling
Plastic hinges were used to model the material non-
linearity. Stress against strain relationships, according to
the EC 2 model [11], were used to model the confined and
the unconfined concrete. XTRACT software[12]was used
to analyse element sections and to calculate flexural load
resistances. Plastic hinge generalised load against deforma-
tion diagrams used for the modelling [1,2,6,13] were
considered to be elastic, perfectly plastic representations
(the yield stage moment, My, equals to the ultimate stage
moment). Twenty interaction diagrams of axial force, N,
against ultimate bending moment were produced so thateach different column plastic hinge could be represented.
The columns had different properties because of differences
in geometry, concrete properties, longitudinal steel or
transverse steel. Each column plastic hinge had its own
axial load bending moment interaction diagram. For the
beams, forty-four pairs of flexural resistances (positive and
negative ultimate moment capacities) were calculated
because every different beam plastic hinge had its own
pair of flexural force resistances. Again, this was because of
differences in concrete properties, longitudinal steel or
transverse steel.
Average values for strength and maximum strain were
used to determine the flexural resistances (loads and
deformations), while characteristic values of the uniaxial
cylindrical concrete strength and the yield stress of the
longitudinal bars [9] were used to determine shear
resistances.
4. Local characteristics
4.1. Comparison of effective yield point rigidities and chord
rotations at yielding
The axial force at each plastic hinge was approximated
by an elastic analysis that took into account the quasi-
permanent gravity loads.
FEMA 356 [1] and ATC 40 [13] suggest modification
factors that decrease the elastic rigidity of the gross
concrete section. These modification factors usually equal
0.5 for columns and beams.
EC 8 [2] and GRECO [6] suggest the following
expression for the effective yield point rigidity:
EIeff My
3yyLs, (1)
where Ls denotes the shear span and yy is the chord
rotation at yielding evaluated from the following European(EC 8[2]and GRECO[6]) semi-empirical expression that is
based on the proposals of Panagiotakos and Fardis[14]:
yy 1=ryLsav z
3 0:0013511:5
h
Ls
y
d d1
db fy
6ffiffiffiffiffifc
p , 2where (1/r)yis the curvature at the yield stage, avis equal to
1 if shear cracking is expected, otherwise av is equal to 0,
zis the length of the internal level arm, h is the depth of the
cross-section, ey is the steel yield strain, d and d1 are the
respective depths to the tension and the compression
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5.0
0
5.0
0
6.00 4.00
Fig. 1. Plan of the bare frame building model [8,9].
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reinforcement, db is the average diameter of the tension
reinforcement, fy is the yield stress of the longitudinal bars
in MPa and fc is the uniaxial cylindrical concrete strength
in MPa.
It is obvious that the European expressions (Eqs. (1) and
(2)) are strongly related to internal axial forces and directly
involve one term for the slippage of longitudinal bars atjoints. The American modification factors do not strongly
take into account internal axial forces, nor do they directly
involve any slippage effect.
Another issue that affects results is the approximation
for the determination of the effective slab width. FEMA
356[1] suggests that the effective flange on each side of the
web of a beam is equal to the smaller of the provided flange
width, eight times the flange thickness, half the distance to
the next web or one-fifth of the span of the beam. GRECO
[6]suggests that the effective flange on each side of the web
is equal to the smaller of the provided flange width, half the
distance to the next web or one quarter of the span of the
beam. It is obvious that GRECO [6] gives slightly larger
values than FEMA 356 [1].
The calculated effective rigidities for columns from the
GRECO [6] procedure ranged from 6.7 103 to
23.8 103 kN m2 while values from the FEMA 356 [1]
procedure ranged from 30.5 103 to 57.4 103 kN m2. In
addition, the calculated effective rigidities for beams from
the GRECO [6] procedure ranged from 9.5 103 to
18.6 103 kN m2, while values from the FEMA 356 [1]
procedure ranged from 63.9 103 to 94.2 103 kN m2.
Fig. 2 presents a comparison of the calculated effective
rigidities of the columns (there are 36 values but some
points coincide because of symmetry) and of the calculatedeffective rigidities of the beams (there are 24 values but
again some points coincide because of symmetry), for the
direction of testing.
It can be seen from Fig. 2 that FEMA 356 [1]
assumptions lead to significantly higher values of EIeff.
For the columns, the average of the ratio of EIeffFEMA/
EIeffGRECO was equal to 3.55 with a standard deviation,s, of
0.72. For the beams, the average of the ratio of EI effFEMA/
EIeffGRECO was equal to 5.88 and s equalled 0.71.
The EC 8[2]and GRECO[6]assumptions correspond to
effective stiffness ratios (the ratio of the effective stiffness
to the elastic stiffness of the gross concrete section) for the
building model that range from 10% to 22% for the
columns and from 6% to 10% for the beams. As stated by
fib [4], values determined by expressions like Eq. (1) are
significantly lower than values implied by codes for thedesign of new buildings [1517].
The chord rotation at element yielding is not required by
the FEMA 356 [1] procedure and is only used in internal
computer program calculations based on the procedure. In
order to make comparisons for this evaluation, the FEMA
356 [1] effective chord rotation at element yielding was
defined by Eq. (1).
The calculatedyy values for columns from the GRECO
[6] procedure ranged from 0.01 to 0.013 rad while values
from the FEMA 356 [1] procedure ranged from 0.002 to
0.007 rad. In addition, the calculated yy values for beams
from the GRECO [6] procedure ranged from 0.011 to
0.016 rad while values from the FEMA 356 [1] procedure
ranged from 0.001 to 0.005 rad. Fig. 3 presents a
comparison of the calculated yy values for the columns
(there are 72 points because each of the 36 columns had 2
plastic hinges and 1 sign as the columns are symmetrical)
and for the beams (there are 96 points because each of the
24 beams had 2 plastic hinges and 2 signs as the beams are
not symmetrical), for the direction of testing.
It can be seen from Fig. 3 that FEMA 356 [1]
assumptions led to lower values. For the columns, the
average of the ratio ofyyeffFEMA/yy
GRECO equalled 0.3 with s
equal to 0.08 and for the beams, the average of the ratio of
yyeffFEMA
/yyGRECO
equalled 0.2 and s equalled 0.06.As demonstrated by Fig. 3, results for yyeff
FEMA are in
disagreement with the assumption of fib [4], which
considers that FEMA 356 [1] implies values for the yield
rotation that are approximately equal to 0.005 rad for RC
beams and columns.
4.2. Comparison of plastic rotations
In order to calculate plastic rotation capacities according
to either the American recommendations or the European
Codes, a pushover analysis must be performed to
determine internal forces (axial and shear) and moments.
More details about the pushover analyses (an iterative
procedure to calculate plastic rotation capacities) can be
found in Section 5 below.
The FEMA 356 [1] procedure provides values for the
plastic hinge rotation capacity of RC elements. These are
given as acceptable limiting values at every performance
level and are a function of the type of element (beam or
column), the reinforcement, the axial and the shear force
levels and the detailing of the RC elements. For this
evaluation, programmed spreadsheets were used to create
an interactive database [18] of plastic hinge capacities, as
determined according to Tables 67 and Tables 68 of
FEMA 356 [1]. Specifically, plastic hinge rotation capa-
ARTICLE IN PRESS
Columns Beams
EIFEMA(X103kNm
2)
55
45
255 20
90
75
60
8.5 18.5
eff
EIFEMA(X103kNm
2)
eff
EIGRECO (X103kNm2)eff
EIGRECO (X103kNm2)eff
Fig. 2. Comparison of EIeff values.
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cities of beams depend on the shear or the flexure
controlled behaviour, the ratio (rr0)/rbal., the spacing
of the stirrups and the ratio V/(bwd(fc)1/2). Plastic hinge
rotation capacities of columns depend on the shear
controlled or the flexure controlled behaviour, the ratio
N/(bdfc), the spacing of stirrups and the ratioV/(bwd(fc)1/2).
In the above equations, Vis the shear force, ris the ratio of
tension reinforcement, r0 is the ratio of the compression
reinforcement, rbal is the ratio that produces balanced
strain conditions andb and bware, respectively, the widths
of the cross-section and the web.
Following on from semi-empirical expressions proposed
by Panagiotakos and Fardis[14], EC 8[2] and GRECO[6]
provide semi-empirical expressions for the ultimate plastic
chord rotation, yupl, and modification factors in order to
convert average values at the ultimate stage to acceptablelimiting values at every performance level.
For beam and columns with a rectangular cross-section,
EC 8 [2] and GRECO [6] suggest the following empirical
relationship:
yupl 0:01450:25n max0:01;o
0
max0:01;o
0:3fc
0:2 Ls
h
0:35
25ars
fywfc
1:275100rd , 3
wheren equalsN/(bhfc),o and o0, respectively, equalrfy/fc
and r0fy/fc,a is a confinement effectiveness factor,rsis the
ratio of transverse reinforcement parallel to the direction of
loading,fywis the transverse reinforcement steel yield stress
and rd is the ratio of diagonal reinforcement in each
diagonal direction.
For the acceptable limit values of Immediate Occupancy,
Life Safety and Collapse Prevention, GRECO [6] suggests
the following relationships:
yIOpllim 0; yLSpllim
0:5yupl=gRd; yCPpllim
yupl=gRd
andgRd 1:8, 4
where IO is Immediate Occupancy, LS is Life Safety and
CP is Collapse Prevention.
It should be noted that the gRd value is used to convert
mean values from Eq. (3) to mean minus one standard
deviation bounds and is used because of the unavoidable
uncertainty of the model.
For this evaluation, spreadsheets were used to create a
database[18]of plastic chord rotation capacities according
to the above expressions. It was decided to use plastic
chord rotation capacities instead of total chord rotation
capacities due to software limitations. The ETABS
computer program [19] provides a model with perfor-
mance-based point hinges at the ends that are rigid plastic.
This model is essential for an evaluation via an event to
event controlled pushover analysis with the ETABS
software[19].
Calculated available plastic chord rotations at the Life
Safety performance level from the GRECO [6] procedureranged from 0.002 to 0.042 rad, while values from the
FEMA 356[1] procedure ranged from 0.015 to 0.02 rad. In
addition, the calculated available plastic chord rotations at
the Collapse Prevention performance level from the
GRECO [6] procedure ranged from 0.003 to 0.083 rad,
while values from the FEMA 356 [1] procedure ranged
from 0.02 to 0.025 rad. Comparisons of available plastic
chord rotations at the local performance levels of the two
procedures that could be considered as similar (Life Safety
and Collapse Prevention) are presented in Figs. 4 and 5.
Specifically, 144 points (36 columns have 2 plastic hinges
and 2 directions of loading) for columns and 96 points (24
beams have 2 plastic hinges and 2 directions of loading) for
beams are presented in Figs. 4 and 5. At the Immediate
Occupancy performance level, FEMA 356 [1] considers
small plastic deformations in the order of 0.01 rad for
beams and 0.005 rad for columns, while GRECO [6]
considers no plastic deformations.
FromFig. 4, it can be seen that, on average, the GRECO
[6]expression for yLSpllimgives lower values than FEMA 356
[1] while, from Fig. 5, on average, the GRECO [6]
expression for yCPpllimgives higher values than FEMA 356
[1]. Even for the case of the Collapse Prevention level, it
can be seen that a small percentage of FEMA 356[1]values
are greater than GRECO [6] values. The above compar-
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Columns
FE
MA
ye
ff
FEMA
ye
ff
0.007
0.004
0.0010.009 0.013 0.017
0.005
0.003
0.0010.010 0.014 0.018
Beams
GRECO
y
GRECOy
Fig. 3. Comparison ofyy values
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isons appear to agree with the statements of fib [4].
According to fib[4], if the values given by FEMA 356 [1],
at the Collapse Prevention level, are meant to be mean, m,
minus one standard deviation bounds, then in some cases,
for well-detailed elements, they provide larger values than
the fib- [4]based expressions. Values given by FEMA 356
[1] could be considered as more conservative than the
values given by the GRECO [6] expression, if they are
meant to be average values (not ms values) at the
ultimate stage. In this case, the GRECO[6]values shown in
Fig. 5should be multiplied by gRd equal to 1.8.
In addition, it is obvious that FEMA 356 [1] values are
generally constant for both columns and beams. In
contrast, the GRECO [6] values appear to be more case
dependent. FEMA 356 [1] tables give the same value for
columns with an axial force ratio (N/(bdfc)) lower than 0.1.
For beams, FEMA 356 [1] tables give slightly different
values because the ratio (rr0)/rbal is controlled by the
section flexural failure mode (failure of steel reinforcement
bars, failure of concrete, etc.). Furthermore, FEMA 356[1]
tables do not strongly relate the plastic rotation capacity to
the amount of transverse steel. The conforming property
that FEMA 356 [1] proposes is a very gross check that
depends on the spacing of the hoops (lower or greater than
d/3) and on the element shear strength provided by these
hoops (lower or greater than three quarters of the design
shear). As can be seen from Eqs. (3) and (4), the European
Codes strongly relate the plastic rotation capacity to the
ratio of the internal axial force to the gross section
compression capacity, as well as the product of the ratio
of the transverse steel parallel to the direction of loading
and the confinement effectiveness factor and the ratio of
yield stress of the transverse steel to the uniaxial cylindrical
concrete strength. In addition, the shear ratio check,
V/(bwd(fc)1/2), proposed by FEMA 356 [1] is not as
sensitive as the shear span ratio factor, (Ls/h)0.35, that is
inherent in Eq. (3) from the European Codes.
5. Pushover analysis
The evaluation of the structural system was performed
via three-dimensional pushover analyses. ETABS software
[19] was used only as a non-linear solver and a graphical
postprocessor because the remainder of the data had been
calculated with either programmed spreadsheets and/or
databases or XTRACT software [12]. Plastic hinges were
used to model the material non-linearity and the ETABS
[19]performance-based event to event strategy was used
for the solution. Geometric non-linearity effects only were
taken partially into account. Specifically, programmed
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Columns Beams0.021
0.019
0.017
0.0150.00 0.02 0.04 0.060.030.020.01
0.014
0.015
0.016
LSFEMA
p
llim
LSFEMA
p
l lim
pllim
LS GERCO pllim
LS GERCO
Fig. 4. Comparison ofyLSpllimvalues.
Columns Beams
CPFEMA
CPFEMA
pllim
pllim
pl l
im
pl l
im
CP GRECO
CP GRECO
0.027
0.025
0.023
0.0210.00 0.05 0.100.04 0.060.020.00
0.019
0.020
0.021
Fig. 5. Comparison ofyCPpllimvalues.
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databases were created for ultimate moment capacities,
chord rotations at element yielding, effective rigidities,
available plastic rotations (at the three performance levels),
shear capacities and element forces from the analysis. All
these databases were interactive [18]. For example, the
database of plastic rotation capacities received the element
forces from the corresponding database in order tocalculate ypl values. For the calculation of ypl capacities,
an iterative procedure must be used to find the final
internal element forces. The software could not manage
such an iterative procedure and this was done externally.
At least three analyses were carried out for each evaluation
and for each direction of loading. An elastic analysis was
performed to first yield, then a non-linear analysis was
carried out using the yplcapacities that had been calculated
according to the elastic element forces and, finally, a non-
linear analysis was performed using the ypl capacities that
had been calculated according to the previous non-linear
analysis.
5.1. Load patterns
According to the technical report [9], the mode shapes
had not significantly changed after the high-level excitation
test. Because of this and because of the fact that the
fundamental mode had a participating mass ratio of
approximately 85%, a modal pattern proportional to the
shape of the fundamental mode was applied in the
direction under consideration (for two signs of loading).
5.2. Determination of the structural performance level
For this paper, it was considered that local performance
levels determined the structural performance level in a
conservative way. That is, the structural performance level
was equal to the worst local performance level of all the
primary elements.
5.3. Seismic demand
Performance-based design procedures propose checking
the structural system for seismic demands from multiple
Seismic Hazard Levels. Similarly, pseudo-dynamic, PsD,
tests were performed for two values of peak ground
acceleration, PGA [8,9].
According to the technical report [9], an artificial
accelerogram was used as a basis for PsD tests. This
accelerogram fitted the response spectrum given by EC 8
[8,9] for soil profile B with 5% damping [9]. The nominal
PGA was considered to equal 0.3 g[8,9].
A low-level PsD test was performed with the reference
signal scaled by 0.4, while a high-level PsD test was
performed with the reference signal multiplied by 1.5[8,9].
The low-level excitation test, with a nominal PGA equal to
0.12 g, was assumed to correspond to the serviceability
limit state[8,9]. The high-level excitation test, with nominal
PGA equal to 0.45 g, was considered to be representative of
the maximum seismic action for which the frame had been
designed [8,9]. The corresponding pseudo-acceleration
spectra of these signals were calculated in order to
determine the demand spectra (for target displacement
calculation).
5.4. Performance point (target displacement) determination
The development of a capacity curve for a structure can
be extremely useful to the engineer. However, for evalua-
tion or for retrofit purposes, the probable maximum
displacement (performance point or target displacement,
dt) for the specified ground motion must be estimated [13].
An estimate of the displacement due to a given seismic
ground motion may be made by using the equal displace-
ment approximation. This approximation is based on the
assumption that the inelastic spectral displacement is the
same as the elastic spectral displacement. Because of the
possible inaccuracy of this approximation, a significant
amount of effort has been expended in the last few years to
develop simplified methods to estimate this displacement
[1,7,13,15,20]. Both FEMA 356[1]and GRECO[6]suggest
the DCM, which is based on a statistical analysis of the
results of time history analyses of single degree of freedom
systems.
The application of the DCM for this exercise was applied
via programmed spreadsheets and/or databases. An
iterative process must be performed in order to calculate
displacements from the DCM, as many variables (for
example, the structural performance level) are unknown. In
addition, bilinear idealisations of base shear against roof
displacement diagrams have to be performed. The equalenergy rule was applied in order to idealise the capacity
curve to the target displacement point. In order to calculate
the areas enclosed by the curve, above and below the
bilinear approximations, the linear part of the curve was
modelled by a linear function while the non-linear part of
the curve was modelled by a polynomial function.
6. Global characteristics
6.1. Effective (secant at yield) stiffness
It was expected that the different assumptions for
effective rigidities (Section 4.1 above) would produce
noticeable differences in the structural stiffness. Table 1
presents the mode periods from the elastic analyses
according to the FEMA 356 [1] and GRECO [6]
procedures.Table 1 also presents the periods measured at
ELSA Laboratory[8,9]from dynamic snap-back tests. As
stated in the technical report [9], different theoretical
models were analysed with different assumptions for the
collaborating slab width (ranging from 0 to the full width),
the initial stiffness (uncracked cross-section, cracked cross-
section) and the inclusion of slippage effect. The range of
calculated values[8,9]from these analyses is also presented
inTable 1.
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From Table 1, it is obvious that GRECO [6] proposalslead to a large underestimation of the structural effective
stiffness. If the demand, in terms of section moments, is a
small portion of section moment capacity at yielding, then
GRECO[6] does not provide a good estimation of element
rigidity because GRECO [6] applies to element yielding.
The FEMA 356 [1] procedure leads to a slight under-
estimation. The proposals of FEMA 356 [1], regarding
effective rigidities, are similar to the assumptions of codes
for the design of new structures and so the conclusions of
this comparison may have a wider application.
6.2. Comparison of capacity curves
Fig. 6 shows a comparison of the calculated capacity
curves (in terms of base shear against roof displacement)
and the test measurements[8,9]for the low-level excitation
test.
FromFig. 6, it is clear that both the FEMA 356[1] and
GRECO[6] procedures are partially in agreement with the
test results[8,9]. Both procedures predicted that the model
structure would not develop plastic deformations but were
unable to predict the value of the experimentally obtained
base shear, Vb, that equalled 594 kN. The FEMA 356 [1]
procedure led to a base shear at target displacement, Vbt,
of 925 kN while the GRECO[6] procedure predicted a Vbt
equal to 321 kN. The FEMA 356 [1] procedure predicted
the initial stiffness of the model structure, while GRECO
[6] appears unable to predict the initial stiffness. The
maximum experimentally obtained displacement of 39 mm
was accurately predicted by both procedures. FEMA 356
[1] led to dt equal to 39.6 mm while GRECO [6] led to dt
equal to 44.0 mm.Fig. 6demonstrates that the FEMA 356[1] modelling assumptions are close to the pre-yield
characteristics of structural systems.
Fig. 7 shows the comparison of the resistances for the
high-level excitation test.Fig. 7also shows the envelope
curve of the experimental values. It is informative to
compare this idealised curve with the calculated curves to
their respective performance points.
As can be seen fromFig. 7, the FEMA 356[1] modelling
assumptions led to an overestimation of the elastic stiffness
of the structure and, because of this, the developed
experimental displacement of 210 mm was underestimated
(dtFEMA 164 mm). The predicted base shear at the target
displacement (VbtFEMA 1242 kN) could be considered to
be close to the experimental value [8,9]of 1442 kN and the
structural performance level was between the Immediate
Occupancy and the Life Safety levels.
Fig. 7also shows that the GRECO [6]procedure led to
an underestimation of the initial stiffness of the structure
and some events of the resistance history are neglected.
However, the target displacement (dtGRECO 181 mm) was
in better agreement with the experimental value [8,9]than
the FEMA 356 [1] prediction. The small difference in the
predicted base shear between the GRECO [6] procedure
(VbtGRECO 1149 kN) and the FEMA 356 [1] procedure
could be considered as negligible. The predicted structuralperformance level was between the Immediate Occupancy
and the Life Safety levels, as was the case with the FEMA
356[1]procedure.
Obviously, the very large difference in effective stiffness
observed from the two procedures does not substantially
ARTICLE IN PRESS
FEMA
GRECO
Targetdisplacement
Experimentalcurve [9] Roof Displacement (m)
Base
Shear
(kN)
1000
600
200
-0.100 -0.050 -0000 0.050 0.100-200
-600
-1000
Fig. 6. Comparison of capacity curves for the low-level excitation test.
FEMA
GRECO
Experimental curve [8,9]
Roof Displacement (m)
BaseShear(kN)
1500
1000
500
-0.6 -0.4 -0.2 0.2 0.4 0.600
-600
-2000
-1500
-1000
Envelope curve
IO level
LSlevel
CPlevel
Target displacement
(after Targ,Disp.)
Fig. 7. Comparison of capacity curves for the high-level excitation test.
Table 1
Comparison of periods
Period (s) Procedure ELSA theoretical and experimental
values [8,9]
FEMA GRECO Theoretical
analyses
Dynamic snap-
back tests
1st mode 0.62 1.10 0.45 0.53 0.53
2nd mode 0.20 0.36 0.17
3rd mode 0.11 0.20 0.10
4th mode 0.08 0.14 0.06
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influence the target displacement. It is worth noting that, in
principle, for periods corresponding to the descending
branch of the design acceleration spectrum, the target
displacement is linearly dependent on the square root of
the stiffness. In general, for most existing buildings, it can
be expected that GRECO [6] provisions will produce
periods that correspond to the descending branch of thedesign spectrum. Moreover, the frequency content of the
pseudo-acceleration spectrum corresponding to the test
accelerogram gave much lower values than the targeted
design spectrum (EC 8[15]) for the GRECO[6] model and
slightly higher values than the targeted design spectrum for
the FEMA [1] model, making target displacements even
closer despite the large difference in the stiffnesses from the
two procedures. It must be noted that the closeness of the
target displacements is a result peculiar to the specific tests.
In order to investigate the generality of the above findings,
additional calculations were performed using the EC 8 [15]
design spectrum instead of the test pseudo-acceleration
sspectrum. The following target displacements were ob-
tained:dtFEMA 38 mm anddt
GRECO 67 mm for the low-
level excitation test and dtFEMA 159 mm and dt
GRECO
273 mm for the high-level excitation test. In addition, if
the design spectrum of EC 8[15]was used, the GRECO[6]
procedure would lead to a more gradual manifestation of
plastic hinges. In other words, by following the GRECO [6]
procedure, more plastic hinges would be created and
greater rotations would occur. Therefore, if the design
spectrum of EC 8[15]was used, the plastic mechanism and
the performance level of the plastic hinges from GRECO
[6]would be closer to the FEMA [1]predictions. It has to
be pointed out that the degree of validity of calculatedresults involving only one time-history of base accelera-
tions is identical to the degree of validity of the test
program.
6.3. Comparison in terms of storey resistances
Fig. 8 presents a comparison of storey drift displacement
profiles at target displacement, dtstorey, for the two procedures
and the experimental maximum storey drift displacements for
the low-level excitation test. The FEMA 356 [1] procedure
predicted drift displacements that had an average of 10%
absolute difference from the experimental values. It could be
considered that the absolute difference (d (Danal.Dexper.)/
Dexper.) was uniformly distributed with storey level
(dstorey1 9%,dstorey2 +9%,dstorey3 7% anddstorey4
13%). The GRECO[6] procedure did not so accurately
predict drift displacements. The average absolute difference
from experimental values was 22% and the difference was
significant non-uniformly distributed (dstorey1 20%,
dstorey2 +20%, dstorey3 +21% and dstorey4 +25%).
Fig. 9presents a comparison of storey drift displacement
profiles at target displacement from the two procedures
and the experimental maximum storey drift displacements
for the high-level excitation test. The FEMA 356 [1]
procedure predicted storey displacements that had an
average of 33% absolute difference from the experimental
values. The difference was not uniformly distributed and its
absolute value increased with the height of the storey level
(dstorey1 16%, dstorey2 25%, dstorey3 37% and
dstorey4 53%). The GRECO [6] procedure predicted
storey displacements that had an average of 21% absolute
difference from the experimental value and the difference
was more uniformly distributed (dstorey1 30%, dstorey2
19%, dstorey3 16% and dstorey4 18%) than
the difference from the FEMA 356 [1] procedure. The
absolute difference decreased as the storey level increased.
For the left and the right loading directions,Figs. 10 and
11 present the deformed shapes and the patterns of the
inelastic mechanism at the target displacement for the high-
level excitation test, for the two procedures, according to
the results of the ETABS software [19]. These figures also
show the ETABS[19]coded state of the plastic hinges. The
ARTICLE IN PRESS
experimental
values [9]
FEMA
procedure
GRECO
procedure
4
3
2
1
00.00 0.01 0.02
Storey Drift Displacement (m)
Storey
Fig. 8. Comparison of storey drift displacement profiles, low-level
excitation test.
experimental
values [8,9]
FEMA
procedure
GRECO
procedure
4
3
2
1
0
0.00 0.01 0.02 0.03 0.04 0.05 0.06 0.07 0.08
Storey Drift Displacement (m)
Storey
Fig. 9. Comparison of storey drift displacement profiles, high-level
excitation test.
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IO coded state indicates that the plastic hinge performance
level was greater than, or equal to, the Immediate
Occupancy performance level and was lower than the Life
Safety performance level. The B coded state indicates that a
plastic hinge developed (the section had yielded) and its
performance level was lower than the Immediate Occu-
pancy performance level. For the GRECO [6] procedure,
there is no B coded state because the yield displacement is
equal to the limit displacement of the Immediate Occu-
pancy performance level. The damage according to the
FEMA 356[1]procedure (12 beam plastic hinges at the B
coded state, 24 beam plastic hinges at the IO coded state, 9
column plastic hinges at the B coded state and 9 column
plastic hinges at the IO coded state) is greater in global
ARTICLE IN PRESS
FEMA
B B B B
B B
BIO IO IO IO
IO IO IO IO
IOIO IO
FEMA
B B B B
B
B
IO IO IO IO
IO IO IO IO
IOIO IO
IO
IO IO
IOIO
IO
IO IO IO
IOIO IO
Experimental [8,9]
Experimental [8,9]GRECO GRECO
IO
Fig. 10. Comparison of the deformed shapes of the internal frame[8,9]and predictions.
FEMA
B B B B
B
B
IO IO IO IO
IO IO IO IO
IOIO IO
FEMA
B B B B
B
B
IO IO IO
IO IO IO IO
IOIO IO
IO
IO IO IO
IO IOIO
IO
IO IO IO
IOIO IO
Experimental [8,9]
Experimental [8,9]GRECO GRECO
Fig. 11. Comparison of the deformed shapes of the external frames[8,9]and predictions.
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terms than the damage according to the GRECO [6]
procedure (30 beam plastic hinges at the IO coded state).
In order to broadly check theoretical predictions, the
middle frames of Figs. 10 and 11 show the experimental
results at the plastic hinge level, where the sizes of the
rhombuses represent (in scale) the size of the maximum
measured total rotation [8,9] for the high-level excitationtest. Because of the fact that the present comparison (at the
plastic hinge level) is performance based, a brief description
of the overall building behaviour during the high-level
excitation test, from the technical report [9], is reproduced
here: During the test, cracks opened (and closed) in the
critical regions of the beams of the first three storeys and of
most of the columns. Only cracks at the beam-to-column
interfaces remained permanently open. Neither spalling of
the cover, nor local instabilities of reinforcement was
observed. Beside the cracks at the beam-to-column inter-
face, which are apparent in the first three storeys and
represent an evidence of local yielding of the rebars, the
specimen remained apparently undamaged. In addition,
the report [9] stated that: The pattern of the maximum
rotations appears to be the one of a weak beam-strong
column mechanism, limited to the first three storeys.
Apparently no plastic hinges took place in the beams of
the external frame at the intersection with the central
column of the second storey. Finally, the report [9] also
stated that: The amount of slippage of the longitudinal
bars in the joint, leading to an increase of both the fixed-
end rotations and the pinching effect.
From Figs. 10 and 11 and from the above brief
description, it is obvious that both procedures predicted
the plastic mechanism and its absence in the fourth storey.Neither the FEMA 356[1] procedure nor the GRECO [6]
procedure predicted the behaviour of the beams of the
external frame at the intersection with the central column
of the second storey. The observed damage, as described in
the technical report [9] and briefly described above, in
terms of local performance levels, could be assumed to be
between the two predictions.
7. Conclusions
The present paper has evaluated the American and
European procedural assumptions for the assessment of
the seismic capacity of existing buildings via pushover
analyses. The FEMA 356- [1] and the Eurocode-based
GRECO [6] procedures have been followed in order to
assess a four-storeyed bare framed building and a
comparison has been made with available experimental
results [9]. The GRECO [6] procedure acts within the
European Code framework and broadly adopts EC 8 [2].
The conclusions of the present study are as follows:
(1) According to FEMA 356 [1] assumptions, effective
yield point rigidities are approximately three times
greater than those of the GRECO [6] procedure for
columns and are roughly five times greater for beams.
This is because effective chord rotations at element
yielding, according to the FEMA 356[1]procedure, are
in the order of one-third the effective chord rotations of
the GRECO [6] procedure for columns and one-fifth
the effective chord rotations for beams. Because of
these differences, there is a large divergence between the
two procedures when approximating the initial stiffnessof the model structure.
(2) The FEMA 356 [1] assumptions are close to the pre-
yield characteristics of structural systems and may be
rationalised for low-level earthquakes. The FEMA 356
[1] predictions of storey drift displacements for such
earthquakes appear to be more consistent with experi-
mental measurements. If the demand, in terms of
section moments, is a low percentage of the capacity,
then the GRECO [6] assumptions underestimated the
initial stiffness of the model structure because they refer
to yielding. However, the range of calculated base shear
values, when compared to the experimental measure-
ments [8,9] was greater for the low-level test than for
the high-level test. For the low-level test, the results
were not controlled by the strength of the structural
elements, which appear to be more predictable than the
rigidities of the structural elements[8,9].
(3) The FEMA 356 [1] available plastic rotations at the
Life Safety performance level are on average greater
than those of GRECO [6], while the opposite happens
for the Collapse Prevention performance level. The
GRECO assumptions appear to be more sensitive to
local characteristics (axial load level, shear force level,
amount of confinement, etc.), while the FEMA 356 [1]
tables give case-independent, steady values. As statedby fib[4], values at the ultimate stage given by FEMA
356 [1] for the case of well-detailed (conforming)
elements could be considered to be more conservative
than values given by the fib-based GRECO [6]
expression, if they are meant to be average values
(not mean minus one standard deviation bounds).
Because of the fact that these values refer to
performance limits (values at the ultimate stage equal
values at the Collapse Prevention level for primary
elements), it could be hypothesised that they are mean
minus one standard deviation bounds.
(4) At high-level excitation, the structural system had a low
rigidity due to slippage of the longitudinal bars at the
joints [8,9]. This phenomenon is directly taken into
account in plastic hinge models only by the GRECO[6]
procedure.
(5) For high-level earthquakes, the FEMA 356 [1] proce-
dure appears to overestimate rigidities and under-
estimate demand deformations. However, the
assumptions for deformation capacities lead the ap-
proach to essentially estimate the structural perfor-
mance level. Undoubtedly, the GRECO [6] procedure
followed a more direct route. Some events of the
resistance history on the capacity curve were neglected
but GRECO [6] essentially predicted the demand
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displacement of the system (performance point). It is
obvious that it also predicted the structural perfor-
mance level. In addition, the GRECO [6]prediction of
storey drift displacements was closer to the experi-
mental results.
(6) For the building under investigation, the GRECO [6]
procedure predicted higher deformations than theFEMA [1] procedure for high and low levels of
excitation. This was also found to be valid when the
EC 8[15]design spectrum was used.
(7) Essentially, both procedures predicted the elasto-plastic
collapse mechanism [8,9] and its storey-to-storey
distribution [9]. Both procedures also predicted the
creation of a plastic hinge in a region that behaved
elastically during the high-level test [9]. In addition, if
the design spectrum of EC 8 [15]was used rather than
the test accelerogram, the GRECO[6]procedure would
predict more plastic hinges and greater rotations.
Therefore, the plastic mechanism and the local
performance levels would be closer to the FEMA [1]
model.
(8) It is clear that, for the building under investigation, the
GRECO [6] procedure gave more reasonable predic-
tions for displacements at high levels of excitation,
while the FEMA [1] procedure gave better predictions
for displacements at low levels of excitation. This
conclusion appears to be valid in the more general case
when the EC 8 [15] design spectrum is used instead of
the test pseudo-acceleration spectrum.
Results of this comparison are only based on theevaluation of one model structure, which may not
represent all RC frame structures. However, although it
appears that the above conclusions could be generalised for
the case of framed RC structures with well-detailed critical
regions (potential plastic hinge regions) and low levels of
axial section forces, further research is required that
investigates other buildings using accelerograms with
different frequency contents.
Acknowledgements
The authors would like to express their gratitude to
ELSA (European Laboratory for Structural Assessment)
for providing the technical report [9] entitled Tests on a
Four-Storey Full-Scale RC Frame Designed According to
Eurocodes 8 and 2 and to Imbsen & Associates, Inc. for
providing a free license for the XTRACT software [12]
within the scope of[18]. In addition, the authors would like
to thank Dr. V. J. Moseley for his invaluable help during
the preparation of this paper.
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