Tsinghua University·Beijing 2012-05-18 Real-time dynamic hybrid testing coupled finite element and shaking table Jin-Ting Wang, Men-Xia Zhou & Feng Jin.

Slides:



Advertisements
Similar presentations
Model-based Real-Time Hybrid Simulation for Large-Scale Experimental Evaluation Brian M. Phillips University of Illinois B. F. Spencer, Jr. University.
Advertisements

Structural Dynamics Laboratory Department of Engineering Science, University of Oxford First European Conference on Earthquake Engineering and Seismology,
An Introduction to Hybrid Simulation – Displacement-Controlled Methods
3-D Dynamic Base Shaking Model 2-D Static BNWF Pushover Model
Mechanics Based Modeling of the Dynamic Response of Wood Frame Building By Ricardo Foschi, Frank Lam,Helmut Prion, Carlos Ventura Henry He and Felix Yao.
PHYS466 Project Kyoungmin Min, Namjung Kim and Ravi Bhadauria.
ADVANCED DYNAMIC TESTING TECHNIQUES IN STRUCTURAL ENGINEERING by Andrei M Reinhorn Xiaoyun Shao CIE 616 FALL 2004.
Reliable Dynamic Analysis of Structures Using Imprecise Probability Mehdi Modares and Joshua Bergerson DEPARTMENT OF CIVIL, ARCHITECTURAL AND EVIRONMENTAL.
ACE2008 ▪ Famagusta ▪ North Cyprus ▪ 15–17 September 2008 ▪ L. Andersen, P. Frigaard & A.H. Augustesen Outline of presentation  Introduction  A two-dimensional.
Structural Qualification Testing of the WindSat Payload Using Sine Bursts Near Structural Resonance Jim Pontius Donald Barnes.
1414 Ball Sound Jakub Chudík Task When two hard steel balls, or similar, are brought gently into contact with each other, an unusual ‘chirping’
MANE 4240 & CIVL 4240 Introduction to Finite Elements Practical considerations in FEM modeling Prof. Suvranu De.
System identification of the brake setup in the TU Delft Vehicle Test Lab (VTL) Jean-Paul Busselaar MSc. thesis.
University of Minho School of Engineering Territory, Environment and Construction Centre (C-TAC) Uma Escola a Reinventar o Futuro – Semana da Escola de.
FE analysis with bar elements E. Tarallo, G. Mastinu POLITECNICO DI MILANO, Dipartimento di Meccanica.
Nazgol Haghighat Supervisor: Prof. Dr. Ir. Daniel J. Rixen
Finite Element Method in Geotechnical Engineering
Characterization of impact damage in fibre reinforced composite plates using embedded FBG sensors J. Frieden*, J. Cugnoni, J. Botsis, Th. Gmür CompTest2011.
M M S S V V 0 Scattering of flexural wave in thin plate with multiple holes by using the null-field integral equation method Wei-Ming Lee 1, Jeng-Tzong.
Team K-TRON Team Members: Ryan Vroom Geoff Cunningham Trevor McClenathan Brendan Tighe.
Feb. 19, 2008 CU-NEES 2008 FHT Workshop Simulation and Control Aspects of FHT M. V. Sivaselvan CO-PI CU-NEES Assistant Professor Dept. of Civil, Environmental.
The Finite Element Method
Finite Element Modeling and Analysis with a Biomechanical Application Alexandra Schönning, Ph.D. Mechanical Engineering University of North Florida ASME.
Streamlined Process for Soil-Structure Interaction Analysis of Nuclear Facilities Utilizing GTSTRUDL and MTR/SASSI Wei Li, Michael Perez, Mansour Tabatabaie,
Solution of Eigenproblem of Non-Proportional Damping Systems by Lanczos Method In-Won Lee, Professor, PE In-Won Lee, Professor, PE Structural Dynamics.
Fifth Tongji-UBC Symposium on Earthquake Engineering REN Xiangxiang Research Institute of Structural engineering and Disaster Reduction 2015/05/04 Dynamic.
Quake Summit 2012 July 9-12, 2012, Boston
Liquefaction Analysis For a Single Piled Foundation By Dr. Lu Chihwei Moh and Associates, Inc. Date: 11/3/2003.
Seyed Mohamad Alavi, Chi Zhou, Yu Cheng Department of Electrical and Computer Engineering Illinois Institute of Technology, Chicago, IL, USA ICC 2009.
Distributed Online Hybrid Test to Trace the Collapse of a Four-Story Steel Moment Frame Tao Wang, IEM, China Andres Jacobsen, Kyoto University, Japan Maria.
FE model implementation of seismically driven GG noise in subterranean gravitational wave detectors David Rabeling, Eric Hennes, and Jo van den Brand
Cheng Chen Ph.D., Assistant Professor School of Engineering San Francisco State University Probabilistic Reliability Analysis of Real-Time Hybrid Simulation.
Static Pushover Analysis
Structural Engineering and Earthquake Simulation Laboratory Experimental and Micromechanical Computational Study of Pile Foundations Subjected to Liquefaction-Induced.
The Finite Element Method A Practical Course
1 SIMULATION OF VIBROACOUSTIC PROBLEM USING COUPLED FE / FE FORMULATION AND MODAL ANALYSIS Ahlem ALIA presented by Nicolas AQUELET Laboratoire de Mécanique.
Haptics and Virtual Reality
LASER and TIG welding ANSYS FE model for thermal and mechanical simulation (A. Capriccioli)
University of Oxford Modelling of joint crowd-structure system using equivalent reduced- DOF system Jackie Sim, Dr. Anthony Blakeborough, Dr. Martin Williams.
Purdue University, West Lafayette, IN Phone: (765) Fax: (765) Investigation of the Effect of Transfer.
1 Real-Time Hybrid Simulations P. Benson Shing University of California, San Diego.
Cheng Chen, Ph.D. Assistant Professor San Francisco State University Interpreting Reliability of Real- Time Hybrid Simulation Results from Actuator Tracking.
July 21, 2005AESE Fast Hybrid Simulation with Geographically Distributed Substructures Gilberto Mosqueda Boza Stojadinovic Jason P. Hanley (Presenter)
Hybrid Simulation of Structural Collapse
Response of a joint passive crowd- SDOF system subjected to crowd jumping load Jackie Sim, Dr. Anthony Blakeborough, Dr. Martin Williams Department of.
The Cosmic Cube Charles L. Seitz Presented By: Jason D. Robey 2 APR 03.
CARE / ELAN / EUROTeV Feedback Loop on a large scale quadrupole prototype Laurent Brunetti* Jacques Lottin**
6/25/20081 Soil-Structure Interaction Analysis of a Composite Structure on a Backfill Hilltop WSRC-STI Rev 0 Lisa Anderson, Bechtel National,
Mahadevan (Lanka) Ilankatharan Adviser: Professor Bruce Kutter
Cracow Grid Workshop, November 5-6, 2001 Concepts for implementing adaptive finite element codes for grid computing Krzysztof Banaś, Joanna Płażek Cracow.
Wireless monitoring of structures Wireless monitoring of structures Monitoring and numerical modeling of Factor building motions Monitoring and numerical.
Pre-focal wave front correction and field stabilization for the E-ELT
Coupling ratio of geophone in the sea bed
1 MIDTERM EXAM REVIEW. 2 m 081.SLDASM REVIEW Excitation force 50N normal to face k=10000N/m m=6.66kg Modal damping 5%
1 Using FE to simulate the effect of tolerance on part deformation By I A Manarvi & N P Juster University of Strathclyde Department of Design Manufacture.
CABER Project Update February 22, 2008
BASICS OF DYNAMICS AND ASEISMIC DESIGN
CTA, MST – seismic calculation Roland Platzer, ZM1 DESY Hamburg Munich, January 28 th, 2013.
ISEC-02 Second International Structural Engineering and Costruction Conference September 22-26,2003, Rome “EVALUATION AND RESULTS’ COMPARISON IN DYNAMIC.
M. Khalili1, M. Larsson2, B. Müller1
IMEKO TC 16 (Pressure) International Conference Cultivating metrological knowledge November, 27 – 30, 2007, Merida, Mexico A 36 MPa PRESSURE BALANCE IN.
PS Internal Dump - actuation system
Th 11 International Conference on Earthquake Resistant Engineering Structures Protection of Masonry Housing in High Seismic Zones with Low-Cost Rubber.
Measurement of Dynamic Properties of Viscoelastic Materials
By Arsalan Jamialahmadi
Status of Target Design
Assessment of Base-isolated CAP1400 Nuclear Island Design
Model Updating of a Nine-Story Concrete Core Wall Building
Implementation of 2D stress-strain Finite Element Modeling on MATLAB
Finite element analysis of effects of asphalt pavement distresses on FWD dynamic deflection basin Qinglong You Jinglian Ma Xin Qiu Chang’an University.
Presentation transcript:

Tsinghua University·Beijing Real-time dynamic hybrid testing coupled finite element and shaking table Jin-Ting Wang, Men-Xia Zhou & Feng Jin

Outlines Introduction to testing system 1 Finite element numerical substructure 2 Single-table testing for soil-structure interaction analysis 3 Dual-table testing for travelling wave effect analysis 4 Summaries 5

1. Introduction to testing system  System framework of Tsinghua real-time dynamic Hybrid testing System (THS) MTS Controller Host PC Ethernet Simulink Host PC Simulink Target PC Etherne t Fibe r Scramn et Control Room Data Acquisition Ethernet Table 1 Table 2 Ethernet

1.1. The shaking table loading system  Two identical uni-axial shaking tables  Working area: 1.5 X1.5 m 2 for each table  Bearing capacity: 2 tone.  The frequency range: 0–50 Hz.  The maximum acceleration: 3.6 g for bare table, 1.2 g for full loaded.

1.2. The distributed real-time calculation system  Real-time calculation system was constructed on a standard PC with the help of xPC TARGET software  Host PC: Develop procedure and debug code  Target PC: Execute real-time calculation

1.3. The shared common RAM network  SCRAMNet cards  The data transfer speed reaches up to 16.7 MB/s  The latency is not more than 250 ns.

1.4. The real-time data acquisition system  Hardware: PXI hardware system  Software: LabVIEW Real-Time Module  The sample rate of single channel can reach 4.4 kHz.

Outlines Introduction to testing system 1 Finite element numerical substructure 2 Single-table testing for soil-structure interaction analysis 3 Dual-table testing for travelling wave effect analysis 4 Conclusions 5

2.1. About FE substructure of RTDHT  Chen and Ricles (2012) developed an independently compiled program named “HybridFEM”.  The program was compiled in Matlab, and can perform FE analysis.  An RTDHT was carried out with the numerical substructure simulated as an FE model with 71 beam elements. Chen C, Ricles JM. Large scale real-time hybrid simulation involving multiple experimental substructures and adaptive actuator delay compensation. Earthquake Engineering and Structure Dynamics 2012; 41(3):

2.1. About FE substructure of RTDHT  Saouma et al. (2012) developed an independently compiled program named “Mercury”.  The program is a set of two identical programs: MATLAB version for instruction, prototyping, and pre-test evaluation; C++ version designed for embedding into real-time system.  Data was interacted by hybrid elements in the program.  An RTDHT was implemented with the numerical substructure simulated as an FE model with 140 flexibility-based elements. Saouma V, Kang DH, Haussmann G. A computational finite-element program for hybrid simulation. Earthquake Engineering and Structure Dynamics 2012; 41(3):

2.2. Our solution to FE substructure  An independently-developed FE analysis block was compiled in S-function.  The new developed block is fully compatible with built-in Simulink blocks.  Don’t need the hybrid elements for data interaction.  Solid elements are used in our FE model.

2.3. Generation of the user-compiled block  The FE analysis program is compiled in C++.  The C++ program is then transplanted into S-function following the special calling syntax.  Finally, the user-compiled block is incorporated into the Simulink procedure to develop the FE numerical substructure.

2.4. Execution of the user-compiled block

2.5. Task Execution Time  The dynamic response of a linear FE model with 66 nodes (132 DOFs) is solved to check the calculation speed of the numerical substructure with FE function.

2.5. Task Execution Time The task execution time  The frequency of the shaking table controller in THS is 1/2048 s.  The task execution time of most simulation steps is about 0.47 ms, but it may significantly increases at a certain step. This leads to the real-time calculation interrupt.

2.5 Task Execution Time  The system management interrupt occasionally occurs in the CPU chip.  A “disableSMI” block is added to the Simulink procedure.  The real-time calculation completed successfully. The task execution time

Outlines Introduction to testing system 1 Finite element numerical substructure 2 Single-table testing for soil-structure interaction analysis 3 Dual-table testing for travelling wave effect analysis 4 Conclusions 5

3.1. Finite soil foundation  A shear frame mounted on the finite soil foundation was tested.

(1) Physical substructure  The upper steel plate mass is 5.28 kg.  White noise excitation shows that the natural frequency of the frame is 4.57 Hz.  The stiffness and damping are calculated as 4350 N/m and N∙s/m, respectively.  It can be considered as a single DOF system in the in-plane movement. Physical substructure

(2) Numerical substructure  50 four-node solid elements, 66 nodes.  A total of 132 DOFs.  The material properties: mass density 2000 kg/m 3 ; elastic modulus 200 MPa; poisson’s ratio 0.2. FE numerical substructure

(3) Acceleration at frame top  The peak of the acceleration at frame top is 0.56 g by RTDHT while 0.49 g by pure FEM, the error is 10.9%.

(3) Acceleration at frame bottom  The peak of the acceleration, at frame bottom is 0.22 g by RTDHT while 0.19 g by pure FEM, the error is 12.1.

(4) Displacement at frame bottom  The peak of the displacement at frame bottom is 4.06 mm by RTDHT while 3.84 mm by pure FEM, the error is 5.4%

3.2. Infinite soil foundation  The foundation is regarded as infinite  The radiation damping is simulated by the viscous- spring artificial boundary.

(1) Effect of the radiation damping  The dynamic response remarkably decreases due to the radiation damping effect of the infinite foundation.  The peak of the acceleration decreases by 43% at frame top and 39% at frame bottom. Acceleration at frame top

(2) Effect of foundation stiffness  The dynamic response under soft soil is considerably smaller than that under hard soil.  The peak of acceleration decreases by 53% at frame top and 60% at frame bottom.  The SSI of different soil conditions differs remarkably. Acceleration at frame top

Outlines Introduction to testing system 1 Finite element numerical substructure 2 Single-table testing for soil-structure interaction analysis 3 Dual-table testing for travelling wave effect analysis 4 Conclusions 5

4.1. Design of the testing  Two shear frames are tested as the physical substructure by two shaking tables.  The foundation is simulated by the FE numerical substructure.

4.2. Physical substructure  The shear frame No.1 used in the experimental substructure is the same as before.  The shear frame No.2 is very similar with No.1. Mass / kgStiffness / N/mDamping / N∙s/m Natural frequency / Hz Damping ratio shear frame No shear frame No

4.3. Numerical substructure  There are 48 four-node solid elements and 65 nodes.  The viscous-spring artificial boundary is set at the truncated boundary.

4.4. Acceleration at the frame top  The dynamic responses of two shear frames have significant phase difference.  The phase difference is about s.  The travelling wave effect has been simulated.

Outlines Introduction to testing system 1 Finite element numerical substructure 2 Single-table testing for soil-structure interaction analysis 3 Dual-table testing for travelling wave effect analysis 4 Conclusions 5

Summaries  An FE analysis block is compiled in S-function. Thus an RTDHT system coupled finite element calculation and shaking table testing is achieved.  The dynamic soil-structure interaction and the travelling wave effect are simulated in RTDHT by using the FE numerical substructure.  The capacity of the real-time hybrid testing is improved due to the FE numerical substructure.

Acknowledgement This research was supported by the National Natural Science Foundation of China (Nos ). The support is gratefully acknowledged.

Thank you for your attention!