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1 Tokyo Institute of Technology | Takeuchi Lab Ben Sitler, PE Arup Unified Method for Floors, Footbridges, Stairs and Other Structures Footfall Induced Vibration

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  • 1 Tokyo Institute of Technology | Takeuchi Lab

    Ben Sitler, PE

    Arup Unified Method for Floors, Footbridges, Stairs and Other Structures

    Footfall Induced Vibration

  • 2 Tokyo Institute of Technology | Takeuchi Lab2

    Outline

    • Introduction to Footfall Induced Vibration• Computing the Structural Response• Project Examples• References

  • 3 Tokyo Institute of Technology | Takeuchi Lab3

    Introduction to Footfall Induced Vibration

  • 4 Tokyo Institute of Technology | Takeuchi Lab4

    When is footfall induced vibration an issue?Introduction to Footfall Induced Vibration

    • Low Frequency (Resonance)• Low Mass (Acc=Force/Mass)• Low Damping• Large Dynamic Loads (Crowds)

  • 5 Tokyo Institute of Technology | Takeuchi Lab5

    The design problemIntroduction to Footfall Induced Vibration :: Loading :: Modal Properties :: Response

    Modal (structural) properties:

    Loading:

    consequences, acceptability, ?????

    • Frequency

    • Modal mass

    • Mode shape

    • Damping

    • Amplitude

    • Frequency

    • Duration

    Response

  • 6 Tokyo Institute of Technology | Takeuchi Lab6

    What does a footfall time history look like?Introduction to Footfall Induced Vibration :: Loading :: Modal Properties :: Response

  • 7 Tokyo Institute of Technology | Takeuchi Lab7

    What kinds of excitation frequencies are possible?Introduction to Footfall Induced Vibration :: Loading :: Modal Properties :: Response

  • 8 Tokyo Institute of Technology | Takeuchi Lab8

    So how does this translate into a design load?Introduction to Footfall Induced Vibration :: Loading :: Modal Properties :: Response

  • 9 Tokyo Institute of Technology | Takeuchi Lab9

    What is an appropriate amount of damping?Introduction to Footfall Induced Vibration :: Loading :: Modal Properties :: Response

    0

    5

    10

    15

    20

    25

    0 0.5 1 1.5 2 2.5 3

    Amplif

    icatio

    n Fact

    or

    (excitation frequency)/(natural frequency)

    Steady State Resonant Amplification Factors for SDOF systems

    0.02 damping0.05 damping0.10 damping0.20 damping

    Damping :: Frequency :: Modal Mass :: Mode Shape

    Be suspicious of >2%

    Footbridges 0.5~1.5%Stairs 0.5%Floors 1~3%

  • 10 Tokyo Institute of Technology | Takeuchi Lab10

    Modelling AssumptionsIntroduction to Footfall Induced Vibration :: Loading :: Modal Properties :: Response

    Damping :: Frequency :: Modal Mass :: Mode Shape

    …some tips (not exhaustive)…Loads Use best estimate, not code values LL: ~0.5kPa typically realistic SDL: upper/lower bound sensitivity studyModel Extent Typically model single floor only Floorplate should capture all modes of interestBoundary Conditions Fixed connections/supports unless true pin Façade vertical fixity may/may not be appropriateMember Modelling Orthotropic slab properties Composite beam (even if nominal studs) Ec,dynamic≈38GPa Subdivide 6+ elements per span

  • 11 Tokyo Institute of Technology | Takeuchi Lab11

    What is a good design criteria?Introduction to Footfall Induced Vibration :: Loading :: Modelling :: Response

    Situation R RMS Acc @ 5Hz

    Low vibration 1 0.005 m/s2

    Residential (night) 1.4 0.007 m/s2

    Residential (day) 2-4 0.01~0.02 m/s2

    Office (high grade) 4 0.02 m/s2

    Office (normal) 8 0.04 m/s2

    Footbridge (heavy) 24 0.12 m/s2

    Footbridge (inside) 32 0.16 m/s2

    Footbridge (outside) 64 0.32 m/s2

    Stair (high use) 24 0.12 m/s2

    Stair (light use) 32 0.16 m/s2

    Stair (very light use) 64 0.32 m/s2

    0.001

    0.01

    0.1

    1 10 100Frequency (Hz)

    rms a

    cceler

    ation (

    m/s2 )

    Approximate threshold of human perception to vertical vibration

    T 2t tRMS RMS

    Acc Peak,HarmonicRMS T

    R=Acc Acc

    AccAcc = =

    2

  • 12 Tokyo Institute of Technology | Takeuchi Lab12

    Computing the Structural Response

  • 13 Tokyo Institute of Technology | Takeuchi Lab13

    Simplified vs Modal vs Time History MethodsComputing the Structural Response

    vs

    vs

    Modal harmonic

    response method

    Explicit time history

    method

  • 14 Tokyo Institute of Technology | Takeuchi Lab14

    Force

    Time

    Analytical ModelComputing the Structural Response

    Py

    cKMy

    Force

    Time

  • 15 Tokyo Institute of Technology | Takeuchi Lab15

    ( ) ( ) ( ) ( ) i tmy t cy t ky t P t P e

    Resonant ResponseComputing the Structural Response

    Py

    cKM

    ,F W DLF f harmonic

    2 2

    2 2 2

    2 22 2 2 2

    1 11 2

    1 21 2 1 2

    h hm m

    h h h hm m m m

    h h h hm m m m

    disp f ff f

    f f f ff f f ff f f ff f f f

    kFRF k m ic i

    i

    SDOF Harmonic Steady State Response

    excition reponseacc

    FAcc FRFm

    …Concrete Centre eq 4.4ƒh = harmonic forcing freq.ƒm = modal (structural) freq.

  • 16 Tokyo Institute of Technology | Takeuchi Lab16

    Transient ResponseComputing the Structural Response

    Force

    Time

    SDOF Impulse – RMS Velocity Response

    ( ) ( ) ( ) ( ) i tmy t cy t ky t P t P e 1.431.354 [Ns]weffn

    fI feff excition reponse

    PeakIVel m

    ( ) sintPeakVel t Vel e t

    ( )RMS mVel RMS Vel t

    ƒw = walking forcing freq.ƒm = modal (structural) freq.…Concrete Centre eq 4.10~4.13

  • 17 Tokyo Institute of Technology | Takeuchi Lab17

    ‘Bobbing’ Resonant ResponseComputing the Structural Response

    122 2

    ( )1 s a s s a a adisp

    a a a a a

    k k m i c c k i cFRF K M iC k i c k m i c

    0 00 0 0 00 0 0 0 0s s s a p a p s s a p a p s

    a a a a a a a ap p p p p p p p

    m y c c c c c y k k k k k y Pm y c c y k k y P

    m y c c y k k y

    22 21(1,1) (1,2) adisp

    aa a s a sa

    mDMF FRF FRF FRF ffk D k D Df f

    2

    1 2a aa a

    f fD if f

    21 2s s

    s s

    f fD if f

    2dispAcc P DMF

    ( ) ( ) ( ) ( ) i tMy t Cy t Ky t P t P e

    ƒ ,aP W GLF harmonic scenario

    MDOF Harmonic Response – crowd interacting with structure

    …IStructE Route 2

    a = active crowdp = passive crowds = structure

  • 18 Tokyo Institute of Technology | Takeuchi Lab18

    Programming ImplementationComputing the Structural Response

    foreach node// Get response of governing excitation frequencyRNode = MAX(RNode(ƒ))foreach excitation frequency// Get R FactorRNode(ƒ) = AccRMS,Node(ƒ) / AccRMS,0(ƒ)// Get SRSS accelerationAccRMS,Node(ƒ) = √(∑Mode∑HarmonicAccRMS(n,m,h,ƒ*h)2)foreach mode// Get modal properties// modal frequency (ƒ), damping (ξ) & mass (m)// displacement at excitation(φne) & response(φnr) nodes// ,ƒm,ξm,mm,φne,φnr,Wm,ρm = ...foreach harmonic// Get harmonic properties// dynamic amplification factor(DLF), harmonic freq (ƒ)DLFƒ,h,ƒm,h = ...// Get RMS accelerationAccRMS(n,m,h,ƒ*h)=RMS(F(ƒm,h,ξm,mm,φne,φnr,DLFƒ,h,Wm,ρm))

    2000 nodes x 20 modes x 4 harmonics x 1.5Hz frequency range = 2.4E7 calculations

    …not practical back in ’90s, hence the simplified methods in AISC DG11, AS 5100-2, etc

    6000 nodes x 40 modes x 2 harmonics x 6Hz frequency range (running) = 2.8E8 calculations

    …Excel VBA is single threaded so no parallel processing…Suggest building with parallel libraries in C#, VB, Python, etc

    Footbridge GSA model

    Library floor GSA model

  • 19 Tokyo Institute of Technology | Takeuchi Lab19

    Some Examples

  • 20 Tokyo Institute of Technology | Takeuchi Lab20

    How can we improve response?Examples

    • Increase Damping• Increase Frequency

    • Increase Stiffness• Decrease Mass

    • Increase Mass• Isolate

  • 21 Tokyo Institute of Technology | Takeuchi Lab21

    Further ReadingQuestions?

    General Structures (Vertical Resonant or Transient of Pedestrians)

    • Concrete Centre CCIP-016 A design guide for Footfall Induced Vibration of Structures• SCI P354 Design of Floors for VibrationStadia & Concert Hall (Vertical Resonance of Bobbing Crowd)

    • IStructE Dynamic Performance Requirements for Permanent Grandstands Subject to Crowd Action

    • C. Jones, A. Pavic, P. Reynold, R. Harrison Verification of Equivalent Mass-Spring-Damper Models for Crowd-Structure Vibration Response Prediction

    High Use Footbridges (Lateral Synchronous Lock in and Vertical Crowd)

    • P. Dallard The London Millenium Footbridge• BSI PD 6688-2:2011 Background to National Annex to BS EN 1991-2: Traffic loads on

    bridges

    • Setra Footbridges: Assessment of Vibrational Behaviour of Footbridges under Pedestrian Loading

    contact: [email protected]