Computer Modeling of Structure to Earthquake Load.pdf

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  • 8/14/2019 Computer Modeling of Structure to Earthquake Load.pdf

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    Computer Modeling of

    Structure to Earthquake Load

    ByJohn Li ([email protected])

    Solutions Research Centre

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    Solutions Research Centre

    How Do Earthquake Affect Buildings

    Earthquake

    Seismic waves Site/soil effects

    Soil-structure

    interaction

    Structural

    response

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    Ground Motion Parameters

    For engineering purposes, three

    characteristics of earthquake motion are ofprimary significance:

    Amplitude

    Frequency content

    Duration of the motion

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    Newton Equation of Motion

    Building codes provide guidelines for: F(t)

    Computation method to solve equation Solution interpretation and design

    [ ]{ } [ ]{ } [ ]{ }xMxCxKtFMatF

    &&& ++=

    =

    )(

    )(

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    Earthquake Analysis Procedure

    Modal/Ritz Vectors Analysis

    Equivalent Lateral Load

    Static Pushover Response Spectrum

    Linear Time History

    Nonlinear Time History

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    Energy Conservation

    Energy is the fundamental in dynamic analysis.

    For earthquake resistant design, try tominimize the mechanical energy.

    Use to evaluate the accuracy of the solution.

    Strain

    Energy+

    Kinetic

    Energy=

    Mechanical

    Energy

    Damped

    Energy

    +Strain

    Energy

    +Kinetic

    Energy

    =Work

    Done

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    Modal Vs Ritz Vectors

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    Equivalent Lateral Force Method

    )1(

    1

    nekn

    j

    jj

    iii F

    HW

    HWF =

    =

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    Response Spectrum Analysis

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    Time History Record

    24538-S2486-94020.06 SANTA MONICA - CITY HALL GROUNDS AT 90 DEG

    3000 POINTS OF ACCEL DATA EQUALLY SPACED AT .020 SEC. (UNITS: CM/SEC/SEC)

    2.321 1.647 .854 -.188 -1.492 -.155 1.559 1.468

    1.468 .234 -1.725 -.507 .331 .014 1.031 1.911

    1.272 -1.191 -.432 .994 1.705 1.341 -1.266 -1.638 -.495 3.286 4.705 -.057 -2.141 .031 2.391 3.937

    3.209 -1.892 -4.787 -.361 4.965 2.778 -.768 -1.933

    -3.859 -1.514 .460 -.759 -3.399 -1.470 5.361 .499

    -3.190 -2.014 -6.361 -.327 5.597 -.284 -6.629 -1.982

    3.192 -3.786 -5.605 -3.604 -3.588 1.536 1.673 .285

    -2.091 -4.786 .461 1.878 6.096 6.154 -.362 -.090

    8.028 15.086 9.537 2.588 -3.574 -1.133 2.995 -5.163

    -12.471 -9.782 -4.950 -5.719 -9.039 -8.594 -7.362 -5.799

    .590 6.948 5.881 1.054 5.206 7.877 .808 -8.184

    -11.273 -6.557 -4.386 -5.915 -8.621 -6.395 4.616 11.018

    7.740 4.030 7.361 13.319 14.179 13.029 12.126 7.768

    1.784 -4.704 -10.645 -15.894 -16.559 -9.928 -4.541 3.332

    10.073 5.642 1.994 5.629 6.987 3.263 -6.605 -14.153 -9.129 .915 .638 -7.667 -9.769 -11.986 -8.324 -4.435

    -7.603 -8.013 -5.754 3.932 17.271 17.645 5.381 2.855

    5.636 6.088 3.796 2.630 6.783 8.365 5.489 2.831

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    Time History Function

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    Time History Analysis

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    Time History Trace

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    Time History Video

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    Nonlinear Time History Analysis

    Full nonlinear behavior may be considered in a time-history analysis using direct integration. P-delta effects,

    large-displacements, and material nonlinearity areavailable. Arbitrary loading may be applied. Applicationsinclude seismic loading, dynamic pushover, andinstability analysis. Most commonly used implicitintegration schemes are available, as well as high-speedexplicit integration for wave propagation, blast, andcollapse problems. Nonlinear direct-integration time-

    history analysis cases can be chained together with othernonlinear time-history or static cases (including stagedconstruction), to address a wide range of applications.

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    Nonlinear NLLink Element

    Linear

    Damper Gap

    Hook Plasitc1

    Isolator1 Isolator2

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    Nonlinear Time History

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    Energy Plots

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    Pushover Curve

    M3 Major Moment

    P Axial

    PMM Axial & Bi-Axial Moments

    S Shear

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    Pushover Hinge Types

    M3 Major Moment

    P Axial PMM Axial & Bi-Axial Moments

    S Shear

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    Pushover Analysis Case

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    Hinge Formation

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    Pushover Curve

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    The Reality!!

    Dynamic Testing and Modelling of Existing Buildings in Hong Kong by Dr

    Ray Su, Prof Adrian Chandler, Prof Peter Lee, Dr Alex To & Mr J H Li.

    1.5401.7892.1232.3362.835Torsion

    TRB Building0.8601.1481.4011.3021.588Y Trans

    BSB Building

    0.5780.6610.7271.2871.622Y Trans

    TTT Building

    321

    Test

    Result

    ModificationsBare

    Frame

    Vibration Period (second)

    Vibration

    Mode

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    Power Spectral Density Analysis

    Power-spectral-density analysis is available to determinethe probabilistic response of a structure due to cyclic

    (harmonic, sinusoidal) loading over a range offrequencies. This is useful for fatigue studies, randomresponse due to earthquakes, and other applications.Multiple loads may be applied at different phase angles,

    and may be correlated or uncorrelated. The structuremay be damped or undamped. Frequency-dependentstiffness and damping (complex impedance) propertiesmay be included for modeling foundations and far-fieldeffects, including radiation damping. Power-spectral-density curves may be plotted for any response quantity,and the integrated expected value is automaticallycomputed.