Dynamic Loads.pdf

download Dynamic Loads.pdf

of 86

Transcript of Dynamic Loads.pdf

  • 7/27/2019 Dynamic Loads.pdf

    1/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    DYNAMIC LOADSThere are two types of forces/loads that may act

    on structures, namely static and dynamic forces.

    Static forces are those that are gradually applied

    and remain in place for longer duration of time.

    These forces are either not dependent on time or

    have less dependence on time.

    Live load acting on a structure is considered as a

    static load because it usually varies gradually in

    magnitude and position.

  • 7/27/2019 Dynamic Loads.pdf

    2/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Similarly moving loads may also be considered

    as statically applied forces.

    Dynamic forces are those that are very much

    time dependent and these either act for smallinterval of time or quickly change in magnitude or

    direction.

    Earthquake forces, machinery vibrations and blast

    loadings are examples of dynamic forces.

    Structural response is the deformation behavior

    of a structure associated with a particular loading.

  • 7/27/2019 Dynamic Loads.pdf

    3/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Similarly, dynamic response is the deformationpattern related with the application of dynamic

    forces.

    In case of dynamic load, response of the

    structure is also time-dependent and hence

    varies with time.

    Dynamic response is usually measured in terms

    of deformations (displacements or rotations),velocity and acceleration.

  • 7/27/2019 Dynamic Loads.pdf

    4/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Dynamic force, F(t), is defined as a force that

    changes in magnitude, direction or sense in muchlesser time interval or it has continuous variation

    with time.

    Impact loadis the other extreme where the load isapplied only for an infinitesimal interval of time with

    some momentum and is considered separate from

    the dynamic loads.

    The variation of a dynamic force with time is called

    history of loading.

    Prescribed dynamic loadingis regularly varying

    loading in which well-defined cycles of loading arerepeated after equal intervals of time.

  • 7/27/2019 Dynamic Loads.pdf

    5/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    F(t)

    t

    Fig. A Typical Dynamic Force.

    Example of prescribed loading is a regularvibration of machinery with a certain amplitude

    and frequency.

  • 7/27/2019 Dynamic Loads.pdf

    6/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Amplitude of vibration is the maximum

    structural displacement during one completecycle of load.

    Frequencyis the number of loading cycles in aunit time (usually one second).

    Types Of Prescribed Loading

    a) Periodic loading

    i) Sinusoidal Loading:ii) Stepped Loading:

    iii) Complex Variation Loading:

  • 7/27/2019 Dynamic Loads.pdf

    7/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    F(t)

    t

    F(t)

    t

    F(t)

    t

    Typical Sinusoidal Loading.

    Typical Stepped Loading.

    Typical Complex

    Variation Loading.

  • 7/27/2019 Dynamic Loads.pdf

    8/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    b) Non-periodic loading

    F(t)

    t

    Typical Impulsive Loading.

    F(t)

    t

    Typical Earthquake Loading.

  • 7/27/2019 Dynamic Loads.pdf

    9/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    EARTHQUAKES

    An earthquake is the vibration of earth produced

    by rapid release of energy from within itself.

    This extra energy may be stored in earth and

    released at intervals due to many different

    phenomena, some of which are as under:1. Plate tectonics.

    2. Volcanic eruptions.3. Atomic explosions.

    4. Collision of massive meteorites with thesurface of earth.

  • 7/27/2019 Dynamic Loads.pdf

    10/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Plate Tectonics

    Crust: Crust is the outermost layer of earth

    consisting of solid material varying in temperature

    from surface temperature to a maximumtemperature of 1000 C. Its thickness under deepoceans is between 4 to 6 km and the thickness

    under continents is approximately 30 to 40 km.

    Mantle: This layer has an approximate thickness

    of 3000 km and consists of semi-solid to plasticmaterial. The temperature ranges from 1000 to

    3500 C.

  • 7/27/2019 Dynamic Loads.pdf

    11/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Outer Core: Outer core is a thickness of

    approximately 2250 km and consists of liquid at atemperature of 3500 to 4000 C.

    Inner Core: The inner core has a radius of

    approximately 1200 km and is a layer of solid

    material at temperature higher than 4000 C.

    The outer layer of earth having a thickness of 100

    km is relatively rigid and is called lithosphere.

    The layer of earth below lithosphere having a

    thickness of 400 km is softer and is called

    asthenosphere.

  • 7/27/2019 Dynamic Loads.pdf

    12/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    The lithosphere acts as rigid plate that moves over

    partly molten asthenosphere.

    According to this theory, lithosphere is cracked in

    places or broken in to smaller pieces or plates.

    This may have happened during initial drying of

    the earth from a molten state.

    There are seven large and several small plates.

    The largest plates are the Pacific plate, the NorthAmerican plate, the Eurasian plate, the Antarctic

    plate, the Indo-Australian plate and the African

    plate.

  • 7/27/2019 Dynamic Loads.pdf

    13/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Plate boundaries

    a) Mid-Oceanic Ridge:

    b) Subduction Zone:

    Further, there are three types of plate boundaries

    depending on the relative movement between thetwo adjoining plates.

    i) Convergent Plate Boundary:ii) Divergent Plate Boundary:

    iii) Transform Plate Boundary:

  • 7/27/2019 Dynamic Loads.pdf

    14/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    According to continental drift theory, all thecontinents were once part of a huge landmass,

    which have slowly moved apart.

    The Indian sub-continent was not a part of Asia.It drifted over millions of years from Australia to

    Asia and the collision produced Himalayas.

    Modern techniques such as GIS and GPS prove

    such movements of continents.

    Faults are cracks which are developed within the

    main plates.

  • 7/27/2019 Dynamic Loads.pdf

    15/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    16/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    17/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    18/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    19/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    20/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    21/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Focus And Epicenter

    The point within the earth along the rupturing

    geological faults where an earthquake originates

    is called the focus orhypocenter.

    The point on the earths surface directly above

    the focus is called the epicenter. Earthquakewaves radiate out from the focus.

    The focal depth is the depth of the hypocenter

    below the epicenter.

    Focal distance is the distance from the

    hypocenter to a given reference point.

  • 7/27/2019 Dynamic Loads.pdf

    22/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Earthquake / Seismic Waves

    The waves originated at the rupture zone are

    called body waves and are of the following two

    types:

    (1) P-Waves or Primary Waves or Dilation

    Waves:

    These waves involve particle movement parallel to

    the direction of propagation of the wave, as shownin Fig.

    The speed of travel of these waves is appr. 1.73

    times greater than the other waves.

  • 7/27/2019 Dynamic Loads.pdf

    23/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    These waves are felt earlier in an earthquake

    and cause relatively less damage.

    There is usually an after-shockat an interval

    during which the other more damaging wavesapproach the area.

    Wave Direction Wave Direction

    Particle Movement

    Particle Movement

    (a) P-Waves (b) S-Waves

  • 7/27/2019 Dynamic Loads.pdf

    24/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    (2) S-Waves or Secondary Waves or Shear

    Waves:

    These waves involve particle movement

    perpendicular to the direction of propagation of thewave (refer the Fig.).

    When body waves reach the ground surface, part

    of these is reflected back while other part

    produces surface waves.

    Surface waves are the waves produced on theearths surface due to an earthquake and are of

    following two types:

    P f D Z hid A Siddi i UET L h

  • 7/27/2019 Dynamic Loads.pdf

    25/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    (1) R-Waves or Rayleigh Waves:These waves produce a circular motion

    analogous to the motion of ocean waves.

    Hence, rotation along with vertical movements

    takes place in case of Rayleigh waves (Fig.).

    Movement of Particles in Rayleigh Waves.

    P f D Z hid A Siddi i UET L h

  • 7/27/2019 Dynamic Loads.pdf

    26/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    (2) L-Waves or Love Waves:

    These waves produce horizontal motion along theground surface transverse to the direction of

    propagation.

    Earthquake magnitude and Richter scale

    Earthquake magnitude is a measure of the energy

    released during an earthquake.

    It defines the size of the seismic event but is not

    related with damage or effect of earthquake at agiven location.

    The magnitude of earthquake is usually measuredon Richter scale, which is a log scale.

    P f D Z hid A Siddi i UET L h

  • 7/27/2019 Dynamic Loads.pdf

    27/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    A magnitude of M5 Richter scale is ten-times

    greater than a magnitude of M4 and isassociated with an increase in energy release of

    31.6 times.

    A magnitude of M5 is 100 times greater than a

    magnitude of M3 scale.

    Earthquake intensity and Mercalli scale

    Intensity is an assessment of the effect of the

    earthquake at a given location and is not directlyrelated to the earthquake magnitude.

    P f D Z hid A Siddi i UET L h

  • 7/27/2019 Dynamic Loads.pdf

    28/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    This is determined not by reading instruments butby observing the effects on structures, human life

    and disturbance to the ground surface.

    Modified Mercalli index is based on the observed

    effects of an earthquake at a specific site.

    P f D Z hid A Siddi i UET L h

  • 7/27/2019 Dynamic Loads.pdf

    29/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Total destruction. Waves seen on ground.XII.

    Almost all structures fall. Bridges wrecked. Very wide cracks in ground.XI.

    Many structures damaged. Ground is badly cracked.X.

    All buildings considerably damaged, many shift off at foundations.Noticeable cracks in ground.

    IX.

    Specially designed structures damaged slightly, others collapse.VIII.

    Everyone runs outdoors. Poorly built structures considerably damaged; slight

    damage elsewhere.

    VII.

    Felt by all; many people run outdoors. Furniture moved, slight damage

    occurs.

    VI.

    Felt by nearly everyone; many people awakened. Swaying trees and poles

    may be observed.

    V.

    Felt indoor by many. Feels like a truck has struck the building.IV.

    Tremor noticed by many, but they often do not realize it as an earthquake.III.

    Felt by very few people.II.

    Felt by almost no one.I.

    EffectMercalli

    Scale

    Prof Dr Zahid A Siddiqi UET Lahore

  • 7/27/2019 Dynamic Loads.pdf

    30/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Main Considerations For Seismic Design

    Design of structures to withstand the maximum

    intensity earthquake is highly expensive and may

    not even be possible due to the following factors:

    1. The magnitude, intensity and other

    characteristics of future earthquakes are notprecisely known.

    2. Stiffer structures attract more earthquakeloads. These structures cannot dissipate

    energy and all the energy is stored in them

    making them unstable.

    Prof Dr Zahid A Siddiqi UET Lahore

  • 7/27/2019 Dynamic Loads.pdf

    31/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    3. Heavier design means more mass of the

    structure. Due to larger mass, moreinertial forces are produced during the

    ground excitation.

    The most common method to design

    earthquake resistant structures is to design for

    mild earthquakes of expected commonoccurrence in the elastic range or in the

    inelastic range with less or no permanent

    deformations.

    Ductility is then provided for maximum expected

    intensity of earthquakes.

    Prof Dr Zahid A Siddiqi UET Lahore

  • 7/27/2019 Dynamic Loads.pdf

    32/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Ductilityis a measure of inelastic deformationsthat may be produced in a structure before its

    collapse.

    Inelastic deformations release energy in the form

    of heat and make the structure stable.

    Permanent deformations may be produced in thestructure with considerable cracking and structure

    may not be useable after a severe earthquake.

    However, the life is saved as the people may

    escape out of the building.

    Prof Dr Zahid A Siddiqi UET Lahore

  • 7/27/2019 Dynamic Loads.pdf

    33/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    In essence the main aim of earthquake resistant

    design is to avoid loss of life and then less loss toproperty is the second criterion.

    It may be tried that the damage is repairable formoderate earthquakes.

    Methods Of Analysis For Earthquake Loading

    1 Free Vibration Analysis

    2 Response History Analysis (RHA)3 Response Spectrum Analysis (RSA)

    4 Equivalent Static orPseudo-Static Load Method

    Prof Dr Zahid A Siddiqi UET Lahore

  • 7/27/2019 Dynamic Loads.pdf

    34/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Related Methods Of Dealing With Earthquakes

    1 Base Isolation Method

    2 Use Of Special Energy Dissipating Devices

    DAMPING

    Damping means the presence of frictional forces

    in the structure, which transforms the mechanicalenergy of system in to other forms of energy,

    such as, heat.

    If damping is completely absent in an ideal

    system, a structure once excited will oscillate

    indefinitely with constant amplitude at its naturalfrequency.

    Prof Dr Zahid A Siddiqi UET Lahore

  • 7/27/2019 Dynamic Loads.pdf

    35/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    The viscous damping forces produced areproportional to the velocity of the piston.

    However, the actual damping in a structure may

    result from looseness of joints, dry friction between

    components (called Coulomb damping), material

    damping (or internal damping found by examining

    the area within the hysteresis loop between

    stresses and acceleration), structural damping

    (general term for all types of damping in astructure) and many other complex causes that

    would lead to nonlinear behavior of the structure.

    Prof Dr Zahid A Siddiqi UET Lahore

  • 7/27/2019 Dynamic Loads.pdf

    36/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Critical Damping (ccr): It is defined as that

    amount of damping due to which a freely excitedsystem does not oscillate but returns to its

    original position in the shortest possible time.

    Damping Ratio Of System ():

    Damping ratio of a system is defined as the ratioof damping present in a system to its critical

    damping. = c / ccr.

    Citical damping coefficient usually ranges

    between 2 to 10% of ccr( = 0.02 to 0.10) for

    actual structures.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    37/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    = 1 critically damped response

    > 1 over-damped response < 1 under- damped response

    EQUIVALENT STATIC LOAD METHOD

    The parameters discussed in the following

    sub-sections are required to be evaluated toget the values of equivalent static loads

    according to UBC-97.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    38/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Seismic Zone Factor (Z)

    The zone factor (Z) is given as a factor of peak

    acceleration with respect to acceleration due to

    gravity (g) and it varies from 0.075 to 0.40.

    The suggested values correspond to recurrence

    interval of 475 years giving a 10 percentprobability of being exceeded in a 50 years

    period.

    0.0750.150.200.300.40Effective Peak Ground

    Acceleration (EPA)

    12A2B34Zone

    Table. Seismic Zones and Effective Peak Ground Accelerations.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    39/86

    q , ,

    Soil Profile Types

    The ground vibrations traveling through the soil

    may be amplified or reduced depending upon the

    fundamental period and type of strata.

    UBC classifies soils into six profile types, as

    given in Table.

    This classification depends on the average shear

    wave velocity in the top 30m of material.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    40/86

    q , ,

    Detailed investigations requiredVery soft clayey soilSF

    < 180Soft soilSE

    180 to 360Stiff soilSD

    360 to 760Soft rockSC

    760 to 1500RockSB

    > 1500Hard rockSA

    Shear Wave Velocity

    (m/s)

    Description of SoilSoil Profile Type

    Table. Soil Profile Types.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    41/86

    q , ,

    Seismic Source Types

    The seismic source types are decided based on

    the maximum moment magnitude potential of a

    fault and its slip rate per year.Type C represents almost an inactive fault in

    Table.

    2.0 6.5C

    The fault which is not A or CB

    5.0 7.0A

    Slip Rate (mm/year)Maximum Moment Potential

    Source CharacteristicsSeismic Source

    Type

    Table. Seismic Source Characteristics.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    42/86

    q

    Near-Source Factors

    Two factors, Na and Nv, are used to considerincreased ground motions near a fault.

    The factorNa is the acceleration-based factorthat is important for short-period structures and

    velocity-based factorNv that is important for

    periods exceeding one second.

    1.01.01.01.01.21.01.61.3B1.01.01.21.01.61.22.01.5A

    Nv

    Na

    Nv

    Na

    Nv

    Na

    Nv

    Na

    15 km10 km5 km 2 kmDistance From FaultSeismic

    Source

    Type

    Table. Near Source Factors (Na

    and Nv) for Various Seismic Source Types.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    43/86

    Ground Response Coefficients

    The two ground response coefficients, Ca and Cv,

    give indication of the vibration amplification

    capacity of a soil depending on zone factor (Z), soilprofile factor (S) and the near-source factors (Naand Nv).

    The fundamental period of a structure determines

    whetherCa orCv is more important for design of a

    structure.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    44/86

    0.96 Nv

    0.36 Na

    0.840.360.640.340.500.300.260.19SE

    0.64 Nv

    0.44 Na

    0.540.360.400.280.320.220.180.12SD

    0.56 Nv

    0.40 Na

    0.450.330.320.240.250.180.130.09SC

    0.40 Nv

    0.40 Na

    0.300.300.200.200.150.150.080.08SB

    0.32 Nv0.32 Na0.240.240.160.160.120.120.060.06SA

    Cv

    Ca

    Cv

    Ca

    Cv

    Ca

    Cv

    Ca

    Cv

    Ca

    Zone 4Zone 3Zone 2BZone 2AZone 1Soil

    Profile

    Table. Ground Response Coefficients, Ca

    and Cv

    .

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    45/86

    When soil parameters are unknown, soil profile

    type SD may be assumed in seismic zones 3 and 4and profile SEmay be assumed in other zones.

    For a regular structure, the near source factor

    needs not exceed 1.3.

    Fundamental Time Period Of A Structure

    The time period of a structure may exactly be

    calculated by performing free vibration analysis of

    the structure, which involves lengthy calculations.

    Following empirical methods are also available to

    reasonably guess the fundamental time period ofa structure:

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    46/86

    Approximate method

    Fundamental time period, T = sec10

    storiesofnumber

    Method A of UBC

    TA =4

    3

    )( nt hC

    wherehn = height of the roof above the base in

    meters, not including the height of parapets.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    47/86

    Ct = 0.085 for steel moment resisting frames

    = 0.073 for reinforced concrete moment

    resisting frames and eccentric braced steel

    frames

    = 0.050 for all other buildings

    Method B of UBC

    TB =

    ii

    ii

    fg

    W

    2

    2

    1.4TA for Zones 1,2 and 3

    1.3 TA for Zones 4

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    48/86

    where

    i = static elastic deflection at level i dueto the forces applied at all levels,

    increasing in a linear way with height.

    The value of deflection must be withrespect to the base in mm.

    = 1floorth-atforcelateraltotal

    + iiki

    ki = shear stiffness of columns under floor i

    fi = lateral force at level i, N

    wi = dead load located at level i, Nand

    g = acceleration due to gravity

    = 9810 mm/sec

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    49/86

    Ductility

    Ductility of an element shows its capacity todeform in the inelastic range without collapse.

    Due to these inelastic deformations, the energyis dissipated making the structure relatively

    stable against earthquake forces.

    If these deformations successfully occur in the

    two opposite directions causing reversal of

    stresses in the members, hysteresis loops areproduced dissipating energy in each cycle of

    loading, unloading and loading in the opposite

    direction.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    50/86

    Response Modification Factor (R)

    The response modification factor of a structure (R)

    is ratio of the seismic base shear of an elastic

    system to a reduced design base shear dependingupon ductility, energy absorbing capacity, increase

    in natural period due to yielding and increase in

    damping ratio of the structure.

    If shear walls or braced frames provide support to

    gravity loads and all the lateral loads, the structuralsystem is a Bearing Wall System (BWS). In other

    words, the gravity loads are resting on walls.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    51/86

    If separate systems are provided to resist lateral and

    gravity loads, the structural system is called BuildingFrame System (BFS).

    No special detailing is required for gravity load

    supporting frames.

    Special Moment Resisting Frames (SMRF) are

    frames specially detailed to provide high ductility andsupport for lateral and gravity loads by flexural action.

    Moment Resisting Frames With Masonry ShearWalls are called MRWFsystems.

    Dual Systems are those in which more than one

    systems are used together.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    52/86

    Many other types given in UBC

    None8.59. Concrete shear walls with SMRF

    496.58. Masonry MRWF

    None8.57. Steel or concrete SMRF

    736.46. BFS with steel ordinary braced frames

    495.55. BFS with masonry shear walls

    735.54. BFS with concrete shear walls

    737.03. BFS with steel eccentrically braced frames

    494.42. BWS with steel braced frames

    494.51. BWS with concrete or masonry shear walls

    Height Limit(m)

    RStructural System

    Table. Response Modification Factor, R.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    53/86

    The value of the response modification factor (R) isdetermined from consideration of a structures

    over-strength capacity beyond the point at which

    the elastic response of the structure is exceeded.

    The value ofRalways exceeds unity, which

    indicates that all structures are designed for forcesless than would be produced in a completely

    elastic structure.

    This reduced force level is made possible by the

    energy absorption and dissipation capacity of the

    structure at displacements in excess of initial yield.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    54/86

    Seismic Importance Factor (I)

    The factor is equal to 1.25 for essential and

    hazardous facilities and 1.00 for special

    occupancy, standard occupancy andmiscellaneous structures.

    Seismic Response Coefficient (Cs

    )

    The seismic response coefficient (Cs) is the

    fraction of total dead load of the structure that is

    acting as base shear on the structure.

    This means that the base shear (V) is: V= Cs W.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    55/86

    This factor depends upon velocity of acceleration

    based ground response coefficient (CvorCa),importance factor (I), response modification factor

    (R) and time period (T).

    Response time Ts =a

    v

    C

    C

    5.2and Ta = 0.2Ts

    Cs =RTICv (ifT> Ts) subjected to maximum

    and minimum values

    Max. value = 2.5 Ca I / R(Controls when T= Ta to Ts)

    Min. value = 0.11 Ca I(OR) 0.8ZNvI / Rfor zone-4

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    56/86

    Seismic Dead Load (W)

    The seismic dead load (W) consists of the

    following:

    i)Dead load of the structure.

    ii)25 percent of the floor live load for storage and

    warehouses.

    iii)A minimum allowance of 50 kg/m2 for movable

    partitions.

    iv)The total weight of permanent equipment and

    fittings.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    57/86

    Magnitude Of Base Shear (V)

    1 UBC refined formula

    Base shearV = Cs WMaximum inelastic displacement m = 0.7 RsWhere s = the displacement corresponding tothe shear V, given above.

    2 UBC simplified formula

    Base shearV = (3.0 Ca / R)W

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    58/86

    This is a conservative formula having the

    following restrictions:

    i)Ordinary occupancy type.

    ii)Light-frame construction not exceeding 3stories.

    iii)Any construction, except bearing wallsystems, but not exceeding two stories.

    Distribution Of Base Shear

    At Various Story Levels

    Shear at a particular story, FX

    =

    ii

    xx

    aW

    aWV

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    59/86

    Where

    V = modal base shearWi= seismic dead load at level-i

    ai= mode shape component at

    level-i for the given modewx= seismic dead load located at

    level-x

    and ax= mode shape component atlevel-x for the given mode

    For uniform distribution of mass over height and

    for first linear mode, the distribution of base

    shear may be simplified as follows:

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    60/86

    FX

    =

    iixx

    hW

    hWV

    1

    Where V1 = base shear corresponding to first

    mode

    hi = height above the base to level-i

    and hx

    = height above the base to level-x

    In order to account for higher mode effects in the

    above expression for long period buildings, anadditional force Ft is added at the top of the

    structure.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    61/86

    Ft

    = 0.07 T V when T> 0.7 sec

    Where V= total base shear

    = Ft+ Fx

    In such cases: FX =

    ii

    xxt

    hW

    hWFV )(

    RESPONSE SPECTRUM ANALYSIS (RSA)

    Spectral response means the maximumdisplacement, velocity or acceleration response.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    62/86

    Pseudo-Acceleration is the maximum

    displacement of the structure multiplied withsquare of natural circular frequency.

    Pseudo-Velocityis the maximum displacementof the structure during an earthquake multiplied

    with the natural circular frequency.

    Sd = spectral displacement

    Sv = spectral velocity

    = Sd

    Sa = spectral acceleration

    = Sv = 2 Sd

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    63/86

    Because of this inter-relationship, all three spectra

    may be plotted on the same graph using tripartiteaxes and logarithmic scales.

    A response curve orresponse spectrum is agraph of the spectral (or maximum) response of a

    range of single-degree-of-freedom oscillators to a

    specified ground motion, plotted against thefrequency or period of the oscillators.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    64/86

    1,000

    500

    200

    100

    50

    20

    10

    0.0550

    0.10 0.20 0.50 1 52 10Time Period, sec (on log scale)

    Spectral Velocity

    (Sv), mm/sec (on

    log scale)

    = 0 % = 2 % = 5 %

    = 10 %

    A Typical Out-of-Scale Response Spectrum.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Procedure To Use Response

  • 7/27/2019 Dynamic Loads.pdf

    65/86

    Procedure To Use Response

    Spectra For SDOF Systems

    The procedure to use response spectrum to calculate

    the earthquake lateral forces for single degree of

    freedom systems is summarized as under:

    i) Calculate angular speed and time period T

    for the structure.

    ii) Estimate the damping ratio, .

    iii) Use applicable response spectrum for aparticular area and find SdorSvorSa (the

    values are inter-convertible) against the time

    period.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    66/86

    iv) Find shear force in each column as:

    S.F = Sd k

    v) Find the total lateral force by adding shear

    forces in all the columns.

    Procedure To Use Response

    Spectra For MDOF Systems

    The procedure to use response spectrum for the

    calculation of the earthquake lateral forces incase of multiple degrees of freedom systems is

    summarized as under:

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    67/86

    1. Calculate angular speed and time period T

    for the desired mode of vibration of the structure.

    2. Find the mode shape ai.

    3. Estimate the damping ratio .

    4. Find Sd, Sv and Sa from the response

    spectrum or calculate others after knowing oneout of these.

    5. Calculate the effective weight as follows:

    WE =( )( )

    2

    2

    ii

    ii

    aW

    aW

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    68/86

    iiii

    aW

    aWV

    6. Calculate the base shear as follows:

    V = WESa / g

    7. Find the lateral force at each level as follows:

    Fi =

    Example : Determine the base shear for the

    fundamental mode with = 0.05. Also determine

    the lateral load at each level for the fundamentalmode.

    = 15.1 rad/sec

    =86.295.1

    00.1

    ia

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    69/86

    Frame For Example.

    880 kg/m2

    880 kg/m2

    590 kg/m2

    30m 30m

    1

    3

    2

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    70/86

    Solution:Dead Loads:

    Level 1 & 3 = (880)(30)(30) = 7770 kN

    Level 2 = (590)(30)(30) = 5209 kN

    = 15.1 rad/sec

    T = 2 / = 0.416 sec

    From the response spectrum, Sv = 350 mm/sec

    Sa = Sv = 5285 mm/sec2 = 5.285 m/sec2

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    71/86

    The calculations are made in Table using the

    following expressions:

    ( )

    ( )

    2

    2

    ii

    ii

    aW

    aW

    ii

    ii

    aW

    aWV

    WE =

    V = WESa / g and Fi =

    9530911324015020749Total527563555222222.8677703

    241119807101581.9552092

    1844777077701.0077701kNkN-mm

    2

    kN-mmmmkN

    Fi

    Wiai

    2Wiai

    ai

    Wi

    Level

    Table. Calculation Sheet For Example.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    ( )2

  • 7/27/2019 Dynamic Loads.pdf

    72/86

    ( )

    ( )91132

    401502

    81.9

    285.517689

    WE =

    = 17689 kN

    = 9530 kNV =

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    73/86

    UBC RESPONSE

    SPECTRUM METHOD

    UBC Design Response Spectrum is an elasticresponse spectrum for 5 percent equivalent

    viscous damping used to represent the dynamic

    effects of the Design Basis Ground Motion forthe design of structures.

    This response spectrum may be developed for a

    site-specific spectrum based on geologic,

    tectonic, seismological and soil characteristics

    associated with a specific site.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    74/86

    Alternatively, the spectrum constructed inaccordance with the spectral shape given in UBC

    using the site-specific values ofCa and Cvand

    multiplied by the acceleration of gravity, 9.815m/sec.2.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    75/86

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    According to UBC 1633 the following

  • 7/27/2019 Dynamic Loads.pdf

    76/86

    According to UBC 1633, the following

    requirements must be satisfied:

    1. Only the elements of the designated

    seismic-force-resisting system need to be

    used to resist design forces.

    2. The individual components should be

    designed to resist the prescribed designseismic forces acting on them.

    3. All building components in Seismic Zones

    2, 3 and 4 shall be designed to resist the

    effects of the calculated seismic forces and

    the effects of gravity loadings from dead,floor live and snow loads.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    77/86

    4. Consideration shall be given to design for

    uplift effects caused by seismic loads.

    5. In Seismic Zones 2, 3 and 4, provision should

    be made for the effects of earthquake forcesacting in a direction other than principal axes.

    6. If the axial load in the column due to seismic

    forces acting in either direction is less than 20 %

    of the column capacity, the orthogonal effects

    may simply be considered by designing for 100% of the design seismic forces in one direction

    plus 30 % of the design seismic forces in the

    perpendicular direction.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    78/86

    7. The combination requiring the greater

    component strength should be used for design.

    8. Alternatively, the effects of the two orthogonal

    directions may be combined on a square root ofthe sum of the squares (SRSS) basis.

    9. When the SRSS method of combining

    directional effects is used, each term computed

    shall be assigned the sign that will result in the

    most conservative result.10. The strength and stiffness of the framing

    between the base and the foundation shall not

    be less than that of the superstructure.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    79/86

    According to UBC 1633.2.7, concrete frames

    that are part of the lateral-force-resisting

    system should conform to the following:1. Should be special moment-resisting

    frames in Seismic Zones 3 and 4.

    2. Should be a minimum of intermediate

    moment-resisting frames in Seismic

    Zone 2.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    80/86

    According to UBC 1631.4.1, response spectrumanalysis is defined as an elastic dynamic analysis

    of a structure utilizing the peak dynamic response

    of all modes having a significant contribution tototal structural response.

    Peak modal responses are calculated using theordinates of the appropriate response spectrum

    curve which correspond to the modal periods.

    Maximum modal contributions are combined in astatistical manner to obtain an approximate total

    structural response.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    81/86

    This condition is considered satisfied by

    demonstrating that for the modes considered, at

    least 90 percent of the participating mass of the

    structure is included in the calculation of responsefor each principal horizontal direction.

    The peak member forces, displacements, story

    forces, story shears and base reactions for eachmode should be combined by recognized methods.

    When three-dimensional models are used foranalysis, modal interaction effects shall be

    considered when combining modal maxima.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

    Reduction of Loads Based On Ductility

  • 7/27/2019 Dynamic Loads.pdf

    82/86

    According to UBC 1631.5.4, the Elastic

    Response Parameters may be reduced for

    purposes of design in accordance with thefollowing items, with the limitation that that the

    corresponding design base-shear should not be

    less than the Elastic Response Base Sheardivided by the value ofR.

    The corresponding reduced design seismicforces shall be used for design.

    Reduction of Loads Based On Ductility

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    83/86

    1. For all regular structures where the ground

    motion representation complies with Ground

    Motion definition of UBC using designspectrum, Elastic Response Parameters

    may be reduced such that the corresponding

    design base shear is not less than 90percent of the base shear determined in

    accordance with Static Force Procedure.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    84/86

    2. For all regular structures where the ground

    motion representation complies with Ground

    Motion definition of UBC using site-specific designspectrum, Elastic Response Parameters may be

    reduced such that the corresponding design base

    shear is not less than 80 percent of the base

    shear determined in accordance with Static Force

    Procedure.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    85/86

    3. For all irregular structures, regardless of the

    ground motion representation, ElasticResponse Parameters may be reduced such

    that the corresponding design base shear is

    not less than 100 percent of the base sheardetermined in accordance with Static Force

    Procedure.

    Prof. Dr. Zahid A. Siddiqi, UET, Lahore.

  • 7/27/2019 Dynamic Loads.pdf

    86/86

    4. The vertical component of ground motion may

    be defined by scaling corresponding horizontal

    accelerations by a factor of two-thirds.Alternative factors may be used when

    substantiated by site specific data. Where the

    Near Source Factor, Na, is greater than 1.0,

    site-specific vertical response spectra should be

    used in place of the factor of two-thirds.