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B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Project 6
Wind-induced Vibrations
of Long-span Bridges
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Introduction
• Long and slender structures
• Light weight
• Low structural damping
2
Motivation
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Introduction
Wind Engineering (Design)
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Vortex Induced Vibrations
CONTESTABILE, Carlo
Università degli studi di Genova, Italy
KENÉZ, Ágnes
Budapest University of Technology and Economics, Hungary
PIERINO, Sonia
Università degli studi di Genova, Italy
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Introduction
Vortex Induced Vibrations
Vortex-induced vibrations (VIV) are resonance phenomena due to
matching vortex shedding frequency and the structural frequency.
Lock-in Resonance
nv ff )2,18,0(
L
Ufv
D
[1] Tajammal Abbas (2016) , PROJECT 6: WIND-INDUCED VIBRATIONS OF LONG-SPAN BRIDGES, Bauhaus Summer School 2016
Motion of the Alconétar Bridge (upper) and its parameters (right) [1]
Self-limiting phenomenon [1]
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Numerical analysis
Vortex Induced Vibrations
Rectangular cross-section
Pentagon cross-section
Rectangular + half-circle cross-section
Rectangular + deflectors cross-section
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Results
Comparison of displacements
Maximum displacement RMS displacement
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Conclusion
Optimazied shape – Halfcircle
Conlusion
• VIV is self-limiting phenomena, not destructive
• Fatigue problems, comfort issues
• Influence of geometrical shape on VIV
Outlook
• TMD can be studied
• Moveable flaps
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Buffeting analysis
ABDOLLAHI, Hossein
Daneshpajoohan Institute of Higher Education, Iran
SHAHGHOLI, Farshad
Daneshpajoohan Institute of Higher Education, Iran
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
DEFINITION AND REFERENCE OBJECT
Buffeting excitation is caused by fluctuating forces induced by inflow
turbulence in the wind field.
Reference object
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
DYNAMICAL PROPERTIES
Structural system and discretization
fV = 0.401 Hz
fL = 0.444 Hz
fT = 0.913 Hz
Distance [m]
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
BUFFETING RESPONSE
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
BUFFETING RESPONSE
Structural Response U=55 m/s, Tu=Tw=10%.
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Flutter
IVANOVIĆ, Nikola
University of Belgrade, Serbia
LUČIĆ, Sanda
University of Josip Juraj Strossmayer Osijek, Croatia
ŠPIRIĆ, Stefan
University of Belgrade, Serbia
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Phenomenon
Flutter
• Coupling of vertical and torsional oscilating mode
• Aeroelastic instability at higher wind speeds
• Can cause ULS if not taken into account
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Reference Object
Lillebælt Suspension Bridge, Denmark
• Total length 1080 m
• Steel box girder deck section
0,5 Hz
0,156 Hz
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Methodology
Analysis Methods
Analysis Methods
1. Fully analytical
2. Forced vibrations
3. Fully coupled CFD simulation
1. Potential flow theory, analytical aerodynamic and structural model
2. Numerical aerodynamic model and analytical structural model
3. Numerical aerodynamic and strucural model
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Results
Forced Vibrations
Heave Pitch
Fully coupled CFD – single slice
Ucr,Theodorsen = 94 m/s
Ucr,Scanlan = 101 m/s
Ucr,CFD = 98 m/s
Critical wind velocities
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Results
Fully coupled CFD – Multi slice
B a u h a u s U n i v e r s i t y W e i m a r
Modelling and Simulation of Structures
Conclusion