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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

    ARTICLE IN PRESS

    www.elsevier.com/locate/soildyn

    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).

    http://www.elsevier.com/locate/soildynhttp://localhost/var/www/apps/conversion/tmp/scratch_4/dx.doi.org/10.1016/j.soildyn.2006.07.001mailto:[email protected],mailto:[email protected],mailto:[email protected],mailto:[email protected],http://localhost/var/www/apps/conversion/tmp/scratch_4/dx.doi.org/10.1016/j.soildyn.2006.07.001http://www.elsevier.com/locate/soildyn
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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

    ARTICLE IN PRESS

    5.0

    0

    5.0

    0

    6.00 4.00

    Fig. 1. Plan of the bare frame building model [8,9].

    V.G. Bardakis, S.E. Dritsos / Soil Dynamics and Earthquake Engineering 27 (2007) 223233224

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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.

    V.G. Bardakis, S.E. Dritsos / Soil Dynamics and Earthquake Engineering 27 (2007) 223233 225

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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-

    ARTICLE IN PRESS

    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

    V.G. Bardakis, S.E. Dritsos / Soil Dynamics and Earthquake Engineering 27 (2007) 223233226

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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

    ARTICLE IN PRESS

    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.

    V.G. Bardakis, S.E. Dritsos / Soil Dynamics and Earthquake Engineering 27 (2007) 223233 227

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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.

    ARTICLE IN PRESS

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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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