Transcript
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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

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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

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Informing Infrastructure Decisions through Large-Amplitude Forced Vibration Testing

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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)

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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

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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

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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.

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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.

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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)

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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

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Envisioned Field Implementation

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

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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.

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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).

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Modeling of DSFSI Problems - Direct and Substructure Methods

Direct Approach

Substructure Approach

Free Field Interaction

(after Wolf, 1985)

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Impedance

Foundation Dynamics Problem – Impedance Functions

F

C Ku

𝒖 =𝑭

𝑲+ 𝒊𝝎𝑪

Rigid and massless foundation

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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

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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)

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Modes of Vibrations

Sliding/SwayingSliding/

Swaying

RockingRocking

Twisting

Vertical

(from Fang, 1991)

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

(from Gazetas, 1983)

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

a0a0

2 4 6 2 4 6

(Luco and Westman 1971, from Gazetas 1983)

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Damping Ratio for Surface Foundations

(from Richart et al., 1970)

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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.

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

2 4 6 a0 2 4 6 a0

(after Kausel and Ushijima, 1979)

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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 Rr

p

s

3

1 1

2

0

3a

R

Vs

0

0w

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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

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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

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

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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

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Bridge Swaying Response Under Horizontal Harmonic Loading

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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

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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

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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

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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

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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

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Fundamental Swaying Frequency Vs. Pier HeightRigid Base

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

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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

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Finite Element Model of Hobson Avenue Bridge

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Fundamental Swaying Mode for Rigid Base

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Finite Element Model of Hobson Avenue Bridge

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Fundamental Swaying Mode for Flexible Base

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Field Implementation Using UTA NHERI Mobile Shakers

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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

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Hobson Avenue Bridge over I-195, Hamilton, NJ

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Hobson Avenue Bridge over I-195, Hamilton, NJ

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Hobson Avenue Bridge over I-195, Hamilton, NJ

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Hobson Avenue Bridge over I-195, Hamilton, NJ

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Geophone Array

MASW (Multichannel Analysis of Surface Waves) Testing

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MASW (Multichannel Analysis of Surface Waves) Testing

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

Swaying Test – Center Pier

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

Swaying Test – Middle of South Span

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

Swaying Test – South Abutment

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T-Rex Mobile Shaker

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T-Rex in Position for Testing

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T-Rex and THMPER

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Geophones and Accelerometers on Bridge Deck

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Central Pier

Sensors

Sensors

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Ground Triaxial Geophone Array

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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?

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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

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Thank You


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