Seismic Response Analysis-3

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    SEISMIC RESPONSE ANALYSISOF

    STRUCTUTRES

    KAUSHIK CHATTERJEE

    DCE (CIVIL), NPCIL

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    Uncoupled Equations of motionUncoupled Equations of motion

    unun--dampeddampedEquation of motion of an un-damped MDOF

    system is

    Substituting from eq. (1), we get,

    Pre-multiplying by the transpose of the nth mode

    shape vector, Tn ,we get,

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    Uncoupled Equations of motionUncoupled Equations of motion

    unun--dampeddampedNow let us introduce new symbols as,

    These are called the normal coordinate

    generalized mass

    , generalized stiffness and

    generalized loadfor mode n respectively.

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    Uncoupled Equations of motionUncoupled Equations of motion

    unun--dampeddamped

    Thus the eqn. of motion of the MDOF system

    can be written as,

    Which is a SDOF system equation of motion for

    mode n.

    We have learnt earlier that,

    Multiplying both sides by we get,

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    Uncoupled Equations of motionUncoupled Equations of motion

    unun--dampeddamped

    Hence, a set of N simultaneous differentialequations which are coupled by the off-diagonalterms in the mass and stiffness matrices, gets

    converted into a set of N independent normal-coordinates equations.

    The dynamic response can be obtained bysolving separately for the response of eachnormal (modal) coordinate and thensuperposing these by eq. 1 to obtain theresponse in the original coordinates. This is

    called ModalSuperposition Method.

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    Uncoupled Equations of motionUncoupled Equations of motion

    dampeddamped

    The damped eqn. of motion is,

    Normal coordinates transformation can be used to

    uncouple the damped equation of motion.

    Using eqn. (1) and pre-multiplying by the transpose

    of the nth mode shape vector, Tn ,we get,

    The orthogonality property causes all componentsexcept the nth mode term in the mass and stiffness

    expressions of the eqn. to vanish.

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    Uncoupled Equations of motionUncoupled Equations of motion

    dampeddampedIf it is assumed that the corresponding

    orthogonality condition applies to the damping

    matrix also, then the above eqn. can be written

    as,

    Or,

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    Uncoupled Equations of motionUncoupled Equations of motion

    dampeddamped

    Where,

    n is the generalized damping ratio for mode n.

    n = cn/cc = cn/2Mn n

    The normal coordinate generalized mass,

    stiffness and load are identical to those for the

    un-damped system.

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    Required to : Obtain time varying response of structures

    due to dynamic excitation. (Example Turbo-

    generator foundation subjected to dynamic

    machine load)

    Generate floor time history & corresponding

    floor response spectra at various floor levels

    of multistoried buildings, which are used toseismically qualify equipments located on that

    particular floor.

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS.

    Ug U

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    In case of seismic excitation of a MDOF system

    (say a multistoried building) the forces

    generated by the seismic excitation within the

    structural members are due to relativedisplacementbetween the stories.

    No external force is applied on the structure assuch.

    .

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    Hence.

    Substituting this in the equation of motion, we

    get

    As the negative sign on the RHS has no real

    significance in case of seismic analysis, it is

    omitted in the subsequent equations.

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    Applying the concept of generalized coordinatesu=z and pre multiplying by

    .

    we get the equation of motion in generalized

    coordinates as

    Where, is called theModal earthquake excitation factor

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    If the natural mode of vibration isthe natural frequency of vibration is

    and the damping ratio is

    The equation of motion for the nth

    mode ofvibration of the idealized multi-storey building

    can be expressed as

    .

    The ratio Ln/Mn is called

    Modal participation factor

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    The solution to this equation can be written interms of the Duhamel integral (damped system)

    Thus the modal displacement is

    The contribution of the nth mode to the

    displacement at jth floor is given by

    , j=1, 2, 3, ., N

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    The deformation or drift in storey j is given by

    the difference of displacements of the floors

    above and below

    Now find out the equivalent lateral force fn(t),

    which, if applied as static forces, would cause

    structural displacements un(t). Thus

    i.e.,

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    If we express the forces in terms of the massmatrix, then

    Thus, the equivalent force at jth floor, which

    causes lateral displacement ujn(t), is

    The inertial force in the structure can be

    determined by a static analysis, applying these

    equivalent lateral forces.

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    TIME HISTORY ANALYSISTIME HISTORY ANALYSIS

    Then the earthquake response of the structureis obtained by combining the modal responses

    in all the modes of vibration.

    The total value of any response r(t), is thecombination of the contribution of all the

    vibration modes to that response quantity

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    Response spectra is a plot of the maximumresponse of a series SDOF system having

    different natural frequencies, for a particular

    value of damping.

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    As the response in each vibration mode can bemodeled by the response of a SDOF system, the

    maximum response in the mode can be directly

    computed from the response spectra.

    In design Max. response, rather than response

    history is required.

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    To evaluate the earthquake response of a MDOF

    system at any time:

    Evaluate the earthquake response integral at

    that time for each significant response mode.

    To evaluate the maximum response:

    Compute the modal response as before, for

    each time during the earthquake history,

    compare them and find the maximumresponse. ---- Time consuming calculation

    involved.

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    Analysis based on ground motion responsespectra comes as an alternative handy tool.

    For each individual mode of the structure, themaximum response can be obtained directly

    from the response spectra.The maximum response in nth mode can beexpressed in terms ofSdn, Svn, and San which arethe ordinates of the displacement, pseudo

    velocity and pseudo acceleration responsespectra respectively, corresponding to thevibration period and damping ratio of the mode.

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    The maximum modal displacement is

    The maximum displacement at the jth floor is

    The maximum drift in the jth storey is

    The maximum lateral force at the j-th floor is

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    The base shear is given by

    Substituting the value of fjn, we get

    The relation between Sdn, Svn, and San is

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    Steps involved: Determine the response spectrum for the

    ground motion if not already available.

    Compute mass and stiffness matrices m and k. Estimate modal damping ratios.

    Solve the eigen value problem to determine

    the natural frequencies and mode shapes.

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    RESPONSE SPECTRUM ANALYSISRESPONSE SPECTRUM ANALYSIS

    Compute the maximum response in individualmodes of vibration by repeating the following

    steps:

    Corresponding to the period and damping

    ratio, read the ordinates Sdn, and San of the

    displacement and pseudo-acceleration

    response spectra of the ground motion.

    Compute floor displacements.

    Compute storey drifts from floor

    displacements.

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    RESPONSERESPONSE SPECTRUM ANALYSISSPECTRUM ANALYSIS

    Compute equivalent lateral forces.Compute internal forces storey shears and

    moments by static analysis of the structuresubjected to equivalent lateral forces.

    Determine an estimate of the maximum ofany response (displacement of a floor,deformation in storey, shear or moment in astorey, etc.) by combining the modal maximafor the response quantity