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  • 7/29/2019 En Curs10 Dsis

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    1

    Structural Dynamics and EarthquakeEngineering

    Course 10

    Design of buildings for seismic action (2)

    Course notes are available for download athttp://www.ct.upt.ro/users/AurelStratan/

    Combination of the effects of the components ofthe seismic action

    Seismic action has components along three orthogonalaxes:

    2 horizontal components

    1 vertical components

    Peak values of ag forhorizontal motion are NOTrecorded at the same time instant

    Peak values of response are NOTrecorded at the same time instant

    0 5 10 15 20 25 30 35 40-2

    -1

    0

    1

    2

    1.62

    timp, s

    acceleratie,m/s2

    Vrancea, 04.03.1977, INCERC (B), EW

    0 5 10 15 20 25 30 35 40-2

    -1

    0

    1

    2

    -1.95

    timp, s

    acceleratie,m/s2

    Vrancea, 04.03.1977, INCERC (B), NS

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    Combination of the effects of the components ofthe seismic action

    Simultaneous action of two orthogonal horizontalcomponents (lateral force or spectral analysis):

    Seismic response is evaluated separately for each direction ofseismic action

    Peak value of response from the simultaneous action of twohorizontal components is obtained by the SRSS combination ofdirectional response:

    Alternative method for combinationof components of seismic actions

    2 2

    Ed Edx EdyE E E= +

    Combination of the effects of the components ofthe seismic action

    When vertical componentis considered as well:

    2 2 2

    Ed Edx Edy EdzE E E E= + +

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    Vertical component

    Vertical component of seismic action shall be consideredwhen vertical peak ground acceleration agv0.25g, and thestructure has one of the following characteristics:

    has horizontal elements spanning over 20 m

    has cantilever elements with a length over 5 m

    has prestressed horizontal elements

    has columns supported on beams

    is base-isolated

    Conceptual design of buildings

    Seismic response of structures subject to considerableuncertainties:

    characteristics of future seismic motions

    diff. between structural models and real structural behaviour

    elastic model inelastic response

    static analysis dynamic behaviour

    Conceptual design of buildings located in seismic areasis necessary, in order to provide an adequate seismicresponse:

    structural simplicity

    uniformity, symmetry and redundancy

    bi-directional strength and stiffness

    torsional resistance and stiffness

    diafragmatic behaviour at storey levels

    adequate foundation

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    Structural simplicity

    Simple, compact, symmetric structures

    Modelling, analysis, design, detailing and construction ofstructures subjected to smaller uncertainties

    Uniformity, symmetry and redundancy

    Structures should be as regular as possible, with auniform plan layout, allowing for a short and directtransmission of inertia forces to lateral resisting system

    Redundancy: failure of a single member does not implyfailure of the whole structure

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    Bi-directional strength and stiffness

    Gravity - force resisting systems Lateral - force resisting systems

    Seismic motion has components on both horizontaldirections

    Structures should have similar strength and stiffnessalong two main directions

    sistem de preluare

    a fortelor laterale

    sistem de preluare a fortelor gravitationale

    Torsional resistance and stiffness

    Seismic forces centre of mass (CM)

    Resisting forces centre of rigidity (CR)

    Torsionally flexible systems large forces anddeformations in perimetral elements

    Conclusion (1): lateral force resisting systems are moreefficient away from the centre of rigidity

    lateral-forceresisting system

    lateral-force

    resisting system

    gravity-force

    resisting system

    gravity-force

    resisting system

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    Torsional resistance and stiffness

    Seismic forces

    centre of mass (CM) Resisting forces centre of rigidity (CR)

    Eccentricity torsion increased displ. and forces

    Conclusion (2): lateral force resisting systems should belocated as symmetrical as possible

    CR=CM CM

    CR

    X

    Y

    DDDD1x

    2x

    DDDD1x

    2x

    Fx Fx

    DDDD1y

    DDDD2y

    e0y

    Storey diaphragms

    Behaviour of floors as rigid diaphragms

    Collect and transmit forces to lateral-force resisting systems

    Lateral-force resisting systems work together

    Especially relevant in case of complex and non-uniform layouts oflateral-force-resisting systems, or combination of such systemsof different stiffness

    F F

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    Foundations

    Design and construction of the foundations and of theconnection to the superstructure shall ensure that thewhole building is subjected to a uniform seismicexcitation

    Recommendations:

    discrete number of structural walls, of different width andstiffness

    box-type or cellular foundation

    individual foundation elements

    foundation slab or tie-beams between these elements

    Criteria for structural regularity

    Structural regularity:

    plan

    elevation

    Regularity of a structure affects: structural model, 2D or 3D

    analysis method, lateral force method or modal responsespectrum analysis

    value of the behaviour factor q, that need to be reduced forstructures irregular in elevation

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    Criteria for regularity in plan

    A symmetrical distribution of stiffness and mass Compact plan configuration, close to a convex polygonal

    shape (set-backs of max 15% from floor area)

    Rigid diaphragms at storey levels

    At each level, in each principal direction of the structure,the eccentricity shall satisfy:

    eox , eoy - the distance between the centre of stiffness and

    the centre of mass, measured in the direction normal tothe direction of analysis consideredrx, ry the square root of the ratio of the torsionalstiffness to the lateral stiffness in each direction

    ("torsional radius")

    eox 0,30 rx

    eoy 0,30 ry

    Criteria for regularity in elevation

    Lateral-force resisting systems shall run withoutinterruption from their foundations to the top of thebuilding

    Mass and lateral stiffness shall be constant or reducegradually with height

    In framed buildings the ratio of the actual storeyresistance to the resistance required by the analysisshould not vary disproportionately between adjacentstoreys

    Stiffness: reductions are no larger than 30% with respectto adjacent storeys

    Strength: reductions are no larger than 20% with respectto adjacent storeys

    Mass: is not larger than 50% of the mass of adjacentstoreys

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    Criteria for regularity in elevation

    Restrictions on setbacks

    Consequences of structural regularity on analysisand design

    *Only if building height is less than 30 m and fundamentalperiod of vibration T1 < 1.50 s

    Plan irregularity: large torsional eccentricities 3Dmodels

    Vertical irregularities: significant contribution of higher

    modes of vibration

    modal response spectrum analysis

    reduced values of behaviour factor

    Reduced valueModalSpatialNONO

    Reference valueModalSpatialYESNO

    Reduced valueModalPlanarNOYES

    Reference value* Lateral forcePlanarYESYES

    Linear-elastic analysisModelElevationPlan

    Behaviour factor (q)Allowed simplificationRegularity

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    Structural model

    The model of the building shall adequately represent thedistribution of stiffness and mass

    Floors that cannot be modelled as infinitely rigid in-plane

    translational masses (only) can be considered lumpedin nodes

    Floors that can be modelled as infinitely rigid in-planestorey masses can be lumped at the centre of mass ofeach storey:

    2 translational components

    1 rotational components

    X

    Y

    Mx

    My

    Mzz

    mxi

    myi

    mi

    CM

    di

    x y iM M m= =

    2

    zz i iM m d=

    Accidental torsional effects

    Uncertainties associated to distribution of storey massesand/or spatial variation of ground motion

    Accidental eccentricity e1i= 0.05 Li

    Spatial structural model:

    CMFx e

    1yLy CM

    Fy

    e1x

    Lx

    X

    Y

    iii FeM 11 =