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    Strong Ground Motion and Conceptof Response Spectrum

    February 2012

    Sudhir K Jain, IIT Gandhinagar

    Sudhir K. Jain February 2012

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    Strong Ground Motions Near-field ground motions

    Usually accelerations

    Engineers

    -0.3

    -0.2

    -0.1

    0

    0.1

    0.2

    0.3

    0 10 20 30 40 50 60 70 80

    Acc

    n.

    (g)

    PGA=0.32g

    Time (seconds)

    EQ Ground Motions

    Sudhir K. Jain Slide 3February 2012

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    Peak Ground Parameters

    Acceleration (PGA) Velocity (PGV)

    Displacement (PGD)

    Sudhir K. Jain Slide 4February 2012

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    (Martinez-Pereira, 1999)

    Maximum Recorded Motion

    Sudhir K. Jain Slide 5February 2012

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    Parameters

    Duration of Significant Shaking Frequency Content

    0 10 20 30 40 50 60

    0.5g

    Time (sec)

    1985 Mexico Earthquake (SCT 1A; N90E)

    1940 Imperial Valley Earthquake (El Centro; S00E)

    1971 San Fernando Earthquake (Pacoima Dam; N76W)

    1991 Uttarkashi Earthquake (Uttarkashi, N75E)

    Characteristics

    Sudhir K. Jain Slide 6February 2012

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    Influence of Magnitude of EQ

    Source mechanism

    Type of faulting

    Distance from source

    Soil/rock medium along travel path

    Local soil site, geology, topology, etc.,. Attenuationwith Distance

    Fault

    Fault

    Characteristics

    Sudhir K. Jain Slide 7February 2012

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    8/42Sudhir K. Jain February 2012 Slide 8

    Accelerogram

    During ground shaking, one can measureground acceleration versus time (accelerogram)using an accelerograph

    Accelerograph is the instrument

    Accelerogram is the record obtained from it Accelerogram is the variation of ground acceleration with

    time (also calledtime history of ground motion)

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    9/42Sudhir K. Jain February 2012 Slide 9

    Typical Accelerograph

    This is a typical analog instrument. These days, digital instruments arebecoming popular (photo from Earthquakesby Bolt)

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    TypicalAccelerograms

    From Dynamics of Structuresby A K Chopra, Prentice Hall

    Time, sec

    Sudhir K. Jain Slide 10February 2012

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    12/42Sudhir K. Jain February 2012 Slide 12

    Response Spectrum (contd)

    Using a computer, one can calculate theresponse of SDOF system with time (timehistory of response)

    Can pickmaximum response of this SDOF

    system (of given T and damping) from thisresponse time history

    See next slide

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    Sudhir K. Jain February 2012 Slide 14

    Response Spectrum (contd)

    Repeat this exercise for different values ofnatural period.

    For design, we usually need only the maximumresponse.

    Hence, for future use, plot maximum responseversus natural period (for a given value ofdamping).

    Such a plot of maximum response versusnatural period for a given accelerogram is calledresponse spectrum.

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    Sudhir K. Jain February 2012 Slide 16

    Response Spectrum (contd)

    Response Spectrum is useful to obtain maximumresponse of any SDOF system for thataccelerogram and for that value of damping.

    See example on next slide

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    Sudhir K. Jain February 2012 Slide 18

    Response Spectrum (contd)

    May repeat the entire process for different values ofdamping

    Velocity response spectrafor N-S component of 1940El Centro record (dampingvalues of 0, 2, 5 and 10%)

    Fig From Housner, 1970Natural Period T (sec)

    MaximumV

    elocity,in/sec

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    Sudhir K. Jain February 2012 Slide 19

    Response Spectrum (contd)

    Unless otherwise mentioned, response spectrumis based on a linear elastic system

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    Sudhir K. Jain February 2012 Slide 20

    Response Spectrum (contd)

    By response we may mean any responsequantity of interest to us, for example: Absolute acceleration of the mass

    Termed asAcceleration Response Spectrum

    Relative velocity of the mass with respect tobase Termed asVelocity Response Spectrum

    Relative displacement of the mass with respectto base Termed asDisplacement Response Spectrum

    Word Spectra is used to denote plural ofSpectrum.

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    Sudhir K. Jain February 2012 Slide 21

    Response Spectrum (contd)

    Since SDOF system responds maximum to thewaves of frequency near its own naturalfrequency,

    Response spectrum is also a very good way to

    characterize the strong ground motion fromengineering view point.

    For instance, relative strength of low frequency versus highfrequency waves

    See example on next slide

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    Sudhir K. Jain February 2012 Slide 22

    Example: Velocity spectra from two accelerograms

    Note that the two response spectra above show very different frequency content. Groundmotion B has more energy at low periods. An expert may be able to make out from thesespectra that B is recorded at a short distance (say 15km) from a small earthquake, while Ais recorded from a large earthquake at a large distance (say 100km) (Fig. edited fromHousner, 1970)

    Natural Period T (sec)

    Velocity,

    ft/sec

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    Sudhir K. Jain February 2012 Slide 23

    Response Spectrum (contd)

    Response spectrum is a very powerful tool. Uses of response spectrum:

    To obtain maximum response of a SDOF system(to the original accelerogram using which

    response spectrum was obtained) To obtain maximum response in a particular

    mode of vibration of a multi degree of freedom(MDOF) system

    It tells about the characteristics of the groundmotion (accelerogram)

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    Sudhir K. Jain February 2012 Slide 24

    Response Spectrum (contd)

    Different terms used in IS:1893 Design Acceleration Spectrum (clause 3.5)

    Response Spectrum (clause 3.27)

    Acceleration Response Spectrum (used in cl.

    3.30) Design Spectrum (title of cl. 6.4)

    Structural Response Factor

    Average response acceleration coefficient (seeterminology of Sa/g on p. 11)

    Title of Fig. 2: Response Spectra for .

    It is better if the code uses the termconsistently.

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    Sudhir K. Jain February 2012 Slide 25

    Smooth Response Spectrum

    Real spectrum has somewhat irregular shapewith local peaks and valleys

    For design purpose, local peaks and valleysshould be ignored

    Since natural period cannot be calculated withthat much accuracy.

    Hence, smooth response spectrum used fordesign purposes

    For developing design spectra, one also needsto consider other issues We will discuss this later.

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    Sudhir K. Jain February 2012 Slide 26

    Smooth Response Spectrum (contd)

    Acceleration Spectra Velocity Spectra Displacement Spectra

    Shown here are typical smooth spectra used in designfor different values of damping

    (Fig. from Housner, 1970)

    Period (sec)Period (sec) Period (sec)

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    Sudhir K. Jain February 2012 Slide 27

    Ground Acceleration (contd...)

    Note the term Peak Ground Acceleration(PGA) is max acceleration of ground.

    Because of deformation in the structure, themotion of its base and the superstructure will be

    different Max acceleration experienced by mass of the

    structure will be different from the PGA (except ifthe structure is rigid)

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    Sudhir K. Jain February 2012 Slide 28

    Ground Acceleration

    ZPA stands for Zero Period Acceleration.

    Implies max acceleration experienced by astructure having zero natural period (T=0).

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    Sudhir K. Jain February 2012 Slide 29

    Zero Period Acceleration

    An infinitely rigid structure Has zero natural period (T=0)

    Does not deform:

    No relative motion between its mass and its base

    Mass has same acceleration as of the ground

    Hence, ZPA is same as Peak GroundAcceleration

    For very low values of period, acceleration

    spectrum tends to be equal to PGA.

    We should be able to read the value of PGAfrom an acceleration spectrum.

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    Sudhir K. Jain February 2012 Slide 30

    Peak Ground Acceleration (contd)

    Average shape of acceleration responsespectrum for 5% damping (Fig. on next slide) Ordinate at 0.1 to 0.3 sec ~ 2.5 times the PGA

    There can be a stray peak in the ground motion;

    i.e., unusually large peak. Such a peak does not affect most of the

    response spectrum and needs to be ignored.

    Effective Peak Ground Acceleration

    (EPGA) defined as 0.40 times the spectralacceleration in 0.1 to 0.3 sec range (cl. 3.11) There are also other definitions of EPGA, but we

    will not concern ourselves with those.

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    Sudhir K. Jain February 2012 Slide 31

    Typical shape of acceleration spectrum

    Typical shape of acceleration response spectrum

    Spectral acceleration at zero period (T=0) gives PGA

    Value at 0.1-0.3 sec is ~ 2.5 times PGA value (for 5% damping)

    PGA = 0.6g0.00

    0.20

    0.40

    0.60

    0.80

    1.00

    1.20

    1.40

    1.60

    1.80

    0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0 4.5

    Period (sec)

    Sp

    ectralAcceleration(g)

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    Sudhir K. Jain February 2012 Slide 32

    What is Design Spectrum

    Seismic Design Force can be specified in termsof Response Spectrum:

    Termed as Design Spectrum

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    Sudhir K. Jain February 2012 Slide 33

    Response Spectrum versus Design Spectrum

    Consider the Acceleration Response Spectrum Notice the region of red circle marked: a slight

    change in natural period can lead to largevariation in maximum acceleration

    Undamped Natural Period T (sec)SpectralAcceleration,g

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    Sudhir K. Jain February 2012 Slide 36

    Design Spectrum (contd)

    Natural vibration period Tn, sec

    SpectralAccelera

    tion,g

    Fig. from Dynamics of Structures by Chopra, 2001

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    Sudhir K. Jain February 2012 Slide 37

    Design Spectrum (contd)

    Design Spectrum is a design specification It must take into account any issues that have

    bearing on seismic safety.

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    Sudhir K. Jain February 2012 Slide 38

    Design Spectrum (contd)

    Design Spectrum must be accompanied by:

    Load factors or permissible stresses that must beused

    Different choice of load factors will give different seismicsafety to the structure

    Damping to be used in design Variation in the value of damping used will affect the design

    force.

    Method of calculation of natural period

    Depending on modeling assumptions, one can get differentvalues of natural period.

    Type of detailing for ductility

    Design force can be lowered if structure has higher ductility.

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    Sudhir K. Jain February 2012 Slide 40

    Soil Effect (contd)

    This variation in ground motion characteristic fordifferent sites is now accounted for through differentshapes of response spectrum for three types of sites.

    SpectralAccele

    rationCoefficient(S

    a/g)

    Period(s)

    Fig. fromIS:1893-2002

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    Design Spectrum for Stiff Structures

    For very stiff structures (T < 0.1sec), ductility is not helpful in

    reducing the design force.

    Actual shape of response spectrum(may be used for higher modes only)

    T(seconds)

    S

    pectralacceleration

    Design spectrum assumes peakextends to T=0

    Concept sometimes used by the codes forresponse spectrum in low period range.

    As a stiff structure getsdamaged during theshaking, its periodelongates i.e., during the same

    ground shaking, a verystiff structure may rideup the ascending partof the graph.

    Codes tend todisallow the reduction

    in force in the periodrange of T < 0.1sec