Transcript
  • 7th New York City Bridge Conference

    August 26-27, 2013

    BRIDGE ENGINEERING ASSOCIATION

    Informing Infrastructure Decisions through Large-Amplitude Forced Vibration Testing

    Nenad Gucunski, Franklin Moon, John DeVitis and Sharef Farrag

    Civil and Environmental Engineering

    Center for Advanced Infrastructure and Transportation (CAIT)

    Brady Cox and Farnyuh Menq – NHERI, The University of Texas at Austin

    NHERI@UTexas Structural Testing WorkshopNew Brunswick, NJ, August 3, 2017

  • Outline

    • NSF EAGER Project – Objectives and general scope of activities

    • Foundation dynamics and dynamic soil-foundation-structure interaction (DSFSI)

    • Numerical simulation of the dynamic response of a bridge-soil system

    • Field implementation using UTA NHERI mobile shakers

  • Informing Infrastructure Decisions through Large-Amplitude Forced Vibration Testing

  • Motivation - Civil Infrastructure Evaluation

    Aging Infrastructures

    – Need for the development of reliable safety assessment approaches

    – Structural-Identification (St-Id) has evolved over the past few decades as a result of:

    • Adoption of sensing technologies (global and local)

    • Development of highly refined simulation models

    • Development of model calibration techniques (both deterministic and probabilistic)

  • Motivation - Civil Infrastructure Evaluation

    Current St-Id for Structure-Foundation Systems

    – Based largely on the response data using various inputs (static loading, wind, temperature changes, pull-release, impact, shakers, etc.)

    – Those low-level demand inputs are leading to responses similar to operational limit states =>the use of such responses to inform the safety assessment of systems under extreme events requires significant extrapolation

  • Motivation - Civil Infrastructure Evaluation

    => Large-amplitude mobile shakers offer significant potential to improve the reliability of St-Id by overcoming low-level mechanisms in a controlled manner

    NH

    ERI

    Mobile

    Shakers

  • NSF EAGER (Early-concept Grants for Exploratory Research) Project

    Overarching Aim

    – To explore and establish the ability of large-amplitude,

    forced vibration testing to reveal the current performance

    and forecast the future system performance of structures,

    with the consideration of dynamic soil-foundation-structure

    effects.

  • NSF EAGER (Early-concept Grants for Exploratory Research) Project

    More Focused Objectives

    – Develop, evaluate, and refine a series of:

    1. Forced vibration testing and control strategies to capture response measurements indicative of key performance attributes of substructure/foundation and superstructure systems

    2. Data interpretation frameworks for structural system identification and assessment

    – Perform a validation of the testing/control strategies and data interpretation frameworks on an operating structure with known substructure, foundation, and soil characteristics.

  • Research Plan

    • Development of Forced-Vibration Testing Strategies

    – Parametric study to examine the correlation between certain measurable responses (both foundation and superstructure) and the foundation/substructure type/condition

    • Development of Data Interpretation Frameworks

    – Model-Free Frameworks - Methods based primarily on data processing, data visualization, and data fitting techniques

    – Model-based Frameworks - Methods that update simulation models of the system being identified, and then employ these to examine behaviors that cannot be directly observed (St-Id)

  • Research Plan

    • Field Implementation and Validation

    – Field implementation of the most promising testing strategies and data interpretation frameworks

    – Since the deployment of large shakers is the easiest to accomplish on bridges (A bridge in Hamilton, NJ was selected as the implementation structure)

    – To be carried out with a UTA NHERI shaker (T-Rex) and dense instrumentation arrays

  • Envisioned Field Implementation

  • Foundation Dynamics and Dynamic Soil-Foundation-Structure Interaction (DSFSI)

  • Objective of Dynamic Soil-Foundation-Structure (DSFS) Interaction Analysis

    The fundamental

    objective of soil-

    foundation-structure

    interaction analysis is to

    evaluate the dynamic

    response by

    encompassing the

    radiation of energy of

    the waves propagating

    into the soil.

  • Effects of Soil and DSFSI on the Response

    • Site amplification of ground motion (earthquake loading).

    • Soil flexibility will effect the flexibility of the overall SFS (Soil-Foundation-Structure) system and, thus, reduce the fundamental frequency. (In comparison to a structure founded on rock.)

    • Radiation of energy through soil will lead to a significantly higher damping. (Exceptions are shallow soil layers.)

    • DSFSI (Dynamic SFS Interaction) increases as soil becomes softer, and the structure becomes more rigid. And vice versa.

    • Generally, DSFSI gives smaller response amplitudes under earthquake and other dynamic loads than modeling on a rigid base. Displacements at the top of a structure may be larger due to rocking of the structure (foundation).

  • Modeling of DSFSI Problems - Direct and Substructure Methods

    Direct Approach

    Substructure Approach

    Free Field Interaction

    (after Wolf, 1985)

  • Impedance

    Foundation Dynamics Problem – Impedance Functions

    F

    C Ku

    𝒖 =𝑭

    𝑲+ 𝒊𝝎𝑪

    Rigid and massless foundation

  • Kvs - static stiffness

    k - stiffness impedance coefficient

    c - damping impedance coefficient

    a0 - dimensionless frequency (wR/Vs)

    Impedances are functions of frequency!

    K K k ia cv vs ( )0 - vertical impedance

    Response of Foundations to Vertical Loading

  • Factors Affecting Dynamic Response of Foundations

    • Soil properties (primarily shear modulus, damping and Poisson’s ratio)

    • Geometry (shape) of the foundation

    • Depth of embedment of the foundation

    • Presence of a rigid base

    • Mode of vibrations (translation or rotation)

    • Dynamics and frequency of loading

    • Foundation flexibility (stiffness)

  • Modes of Vibrations

    Sliding/SwayingSliding/

    Swaying

    RockingRocking

    Twisting

    Vertical

    (from Fang, 1991)

  • Static Stiffness for a Rigid Circular Footing on an Elastic Half-Space

    (from Gazetas, 1983)

  • Impedance Coefficients for a Circular Footing on an Elastic Half-Space - Vertical

    a0 a02 4 6 2 4 6

    (Luco and Westman 1971, from Gazetas 1983)

  • Damping Ratio for Surface Foundations

    (from Richart et al., 1970)

  • Some Elements Affecting Foundation Impedance Functions

    • Embedment significantly increases the dynamic stiffness and equivalent damping ratio. => An effective way to reduce the anticipated high amplitudes of vibrations.

    • For a foundation on a stratum, static stiffness in all modes increases (more for translational than rotational modes) with the relative radius to depth to bedrock ratio R/H.

    • Impedance coefficients have undulations (instead of smooth functions for H-S) associated with natural frequencies of the stratum.

    • Below the first resonant frequency of each mode of vibration, c is zero or negligible. (No surface waves to radiate energy, while bedrock prevents “vertical” radiation.) Vertical and sliding modes affected more.

    • Foundation flexibility affects soil reaction and displacement distributions, and impedance coefficients.

  • Impedance Coefficients of a Rigid Circular Foundation on a Stratum - Vertical

    2 4 6 a0 2 4 6 a0

    (after Kausel and Ushijima, 1979)

  • Effect of Foundation Flexibility Expressed Through Stiffness Ratio on Soil Reaction Distribution

    0 0.2 0.4 0.6 0.8 1 1.2-2.5

    -2

    -1.5

    -1

    -0.5

    0N

    orm

    alli

    ze

    d s

    oil

    rea

    ctio

    n

    REAL PART =0.0%

    =0.35

    a =2.69

    0

    =0.0

    Normalized radius

    s =0.008 s =0.125 s =1 s =8 s =125r r r r r

    sE h

    V Rrp

    s

    3

    1 1

    2

    0

    3a

    R

    Vs

    0

    0w

  • 0 0.2 0.4 0.6 0.8 1 1.2-0.2

    -0.1

    0

    0.1

    0.2N

    orm

    aliz

    ed d

    ispla

    ce

    me

    nt

    REAL PART

    s =0.008 s =0.125 s =1 s =8 s =125r r r r r

    =0.0%

    =0.35

    a =2.69

    0

    =0.0

    Normalized radius

    Effect of Stiffness Ratio on Displacement Distribution

  • 0 1 2 3 4 5 6 7-2

    -1.5

    -1

    -0.5

    0

    0.5

    1

    1.5

    Dimensionless frequency, a 0

    V

    V

    s1

    s2

    V =2

    =0.35 =0.0 =0.0

    R /d =10 1

    s2

    _

    s =0.008 s =0.125 s =1 s =8 s =125r r r r r

    Impedance c

    oeff

    icie

    nt k

    Effect of Stiffness Ratio on Impedance Functions

  • Numerical Model and Parametric Study of Dynamic Response of Bridge-Soil Systems

  • Parametric Study - 2D Model of Hypothetical Bridge

    Variables

    Vs: Soil S-Wave Velocity; 200-400 m/s

    R: Footing Radius; 2-4 m

    Hc: Column Height; 3-12 m

    Constants

    Wf: Footing Width; 1.3m

    Tf: Footing Thickness; 0.5 m

    Wc: Column Width; 0.5 m

    Ts: Slab Thickness; 0.2 m

    Fs: Half Column Spacing, 3 m

    ρs: Soil Density; 1900 kg/m3

    ν : Poisson’s ratio; 0.333

    Foundation3 m 6 m 3 m

  • Bridge Swaying Response Under Horizontal Harmonic Loading

  • Sample Displacement Time Histories - Deck

    -1.50E-04

    -1.00E-04

    -5.00E-05

    0.00E+00

    5.00E-05

    1.00E-04

    1.50E-04

    2.00E-04

    2.50E-04

    0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5

    Ux

    (m)

    Time (s)

    -3.00E-05

    -2.00E-05

    -1.00E-05

    0.00E+00

    1.00E-05

    2.00E-05

    3.00E-05

    0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5

    Uy

    (m)

    Time (s)

    Horizontal

    Vertical

  • Sample Displacement Time Histories - Foundation

    -1.50E-05

    -1.00E-05

    -5.00E-06

    0.00E+00

    5.00E-06

    1.00E-05

    1.50E-05

    2.00E-05

    2.50E-05

    3.00E-05

    0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5

    Ux

    (m)

    Time (s)

    -0.005

    -0.004

    -0.003

    -0.002

    -0.001

    0

    0.001

    0.002

    0.003

    0 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5

    Ro

    tati

    on

    (ra

    ds)

    Time (s)

    Horizontal

    Rotation

  • 0

    2

    4

    6

    8

    10

    12

    0 0.5 1 1.5 2 2.5 3 3.5 4

    Load

    (kN

    )

    Frequency (Hz)

    Sample Loading Spectrum

  • Sample Horizontal Displacement, Velocity and Acceleration Response Spectra

    -0.01

    -0.005

    0

    0.005

    0.01

    0 1 2 3 4 5

    Dis

    pla

    cem

    ent

    (m)

    Frequency (Hz)-0.00006

    -0.00005

    -0.00004

    -0.00003

    -0.00002

    -0.00001

    0

    0.00001

    0 1 2 3 4 5

    Dis

    pla

    cem

    ent

    (m)

    Frequency (Hz)

    -0.0002

    0

    0.0002

    0.0004

    0.0006

    0.0008

    0.001

    0.0012

    0 1 2 3 4 5

    Vel

    oci

    ty (

    m/s

    )

    Frequency (Hz)-0.005

    0

    0.005

    0.01

    0.015

    0.02

    0 1 2 3 4 5

    Vel

    oci

    ty (

    m/s

    )

    Frequency (Hz)

    -2

    -1.5

    -1

    -0.5

    0

    0.5

    1

    1.5

    2

    2.5

    0 1 2 3 4 5

    Acc

    ele

    rati

    on

    (m

    /s^2

    )

    Frequency (Hz)-0.005

    0

    0.005

    0.01

    0.015

    0.02

    0 1 2 3 4 5Acc

    ele

    rati

    on

    (m

    /s^2

    )

    Frequency (Hz)

    Real Part Imaginary Part

  • Sample Foundation Vertical Displacement and Rotation Response Spectra

    Vertical Displacement

    0.00E+00

    2.00E-02

    4.00E-02

    6.00E-02

    8.00E-02

    1.00E-01

    1.20E-01

    1.40E-01

    1.60E-01

    0 0.5 1 1.5 2 2.5 3 3.5 4

    Uy

    (m)

    Frequency (Hz)

    0.00E+00

    2.00E-04

    4.00E-04

    6.00E-04

    8.00E-04

    1.00E-03

    1.20E-03

    1.40E-03

    1.60E-03

    1.80E-03

    2.00E-03

    0 0.5 1 1.5 2 2.5 3 3.5 4

    Ro

    tati

    on

    (ra

    ds)

    Frequency (Hz)

    Rotation

  • Fundamental Swaying Frequency Vs. Pier HeightRigid Base

  • Fundamental Swaying Frequency Vs. Pier HeightFlexible Base (R=2 m, Vs=200 m/s)

  • Fundamental Swaying Frequency Vs. Slenderness Ratio

    0

    0.5

    1

    1.5

    2

    2.5

    3

    0 0.5 1 1.5 2 2.5

    Fre

    qu

    en

    cy a

    t p

    eak

    (H

    z)

    Slenderness Ratio

    R=2, V=200

    R=2, V=300

    R=3, V=200

    R=3, V=200

    R=3, V=300

    R=3, V=400

    R=4, V=200

    R=4, V=300

    R=4, V=400

    R=8, V=800

  • Finite Element Model of Hobson Avenue Bridge

  • Fundamental Swaying Mode for Rigid Base

  • Finite Element Model of Hobson Avenue Bridge

  • Fundamental Swaying Mode for Flexible Base

  • Field Implementation Using UTA NHERI Mobile Shakers

  • Field Implementation and Validation

    • Objectives :

    – To measure the response of all components: ground, foundation, substructure and superstructure in both vertical and horizontal directions, to infer the contributions of soil-foundation-substructure interaction on the overall response of the superstructure.

    – To enable assessment of transmissibility (motion transfer) and force transfer between superstructure and foundation, and from the foundation to surrounding soil.

    – To enable assessment of foundation impedance functions for both vertical and rocking motion.

    • The results will be compared against the models within the parametric study to place the field test in context

    • Secondary objective: The results obtained from the bridge excitation using a NHERI shaker (vertical mode only) and THMPER will be compared

  • Hobson Avenue Bridge over I-195, Hamilton, NJ

  • Hobson Avenue Bridge over I-195, Hamilton, NJ

  • Hobson Avenue Bridge over I-195, Hamilton, NJ

  • Hobson Avenue Bridge over I-195, Hamilton, NJ

  • Geophone Array

    MASW (Multichannel Analysis of Surface Waves) Testing

  • MASW (Multichannel Analysis of Surface Waves) Testing

  • T-Rex positionDeck Triaxial AccelerometersSubstructure and Ground Triaxial GeophonesDeck Triaxial Geophones

    Swaying Test – Center Pier

  • T-Rex positionDeck Triaxial AccelerometersSubstructure and Ground Triaxial GeophonesDeck Triaxial Geophones

    Swaying Test – Middle of South Span

  • T-Rex positionDeck Triaxial AccelerometersSubstructure and Ground Triaxial GeophonesDeck Triaxial Geophones

    Swaying Test – South Abutment

  • T-Rex Mobile Shaker

  • T-Rex in Position for Testing

  • T-Rex and THMPER

  • Geophones and Accelerometers on Bridge Deck

  • Central Pier

    Sensors

    Sensors

  • Ground Triaxial Geophone Array

  • What Are the Questions We Are Trying to Answer?

    • Can we infer the contributions of soil-foundation-substructure interaction on the overall response of the superstructure?

    • Can we develop data interpretation frameworks for structural system identification and assessment that will take into consideration DSFSI?

    • Can large-amplitude, forced vibration testing using NHERI shakers (in a fully controlled manner) reveal the performance of structures beyond operational limit states? Are we entering a nonlinear range?

  • Acknowledgements

    • NSF EAGER– Project support through Award Id. 1650170 (Program officer: Dr. Richard J. Fragaszy)

    • NSF NHERI (Natural Hazards Engineering Research Infrastructure) – Provided access to UTA NHERI mobile shakers

    • NJDOT – Support in bridge selection, and providing documentation and access to Hobson Avenue Bridge (Mr. Eddy Germain)

    • UTA NHERI team

  • Thank You


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