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University of Oxford Modelling of joint crowd-structure system using equivalent reduced- DOF system Jackie Sim, Dr. Anthony Blakeborough, Dr. Martin Williams Department of Engineering Science Oxford University
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University of Oxford Cantilever grandstands
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University of Oxford Dynamic analysis of cantilever grandstand Human-structure interaction Passive crowd Crowd model Active crowd Load model
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University of Oxford Full model m s F x Total mass of crowd = m s m s F x Crowd as 2DOF system Structure as SDOF system
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University of Oxford Equivalent reduced DOF systems Equivalent SDOF system Equivalent 2DOF system m s F x Full model
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University of Oxford Contents Crowd model Response of full model Equivalent SDOF model Equivalent 2DOF model
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University of Oxford DOF 2 m2m2 k 2 c 1 k 1 m1m1 c 2 m 0 F y2y2 y 1 DOF 1 m2m2 k 2 c 1 k1 k1 m1m1 c 2 F y 2 y 1 DOF 2 Seated model Standing model Individual models – Griffin et al.
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University of Oxford Crowd response
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University of Oxford Crowd model Transfer functions: Seated: Standing: Fourth order polynomial i.e. 2DOF system
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University of Oxford Dynamic analysis (1) 2% structural damping, Natural frequency of 1 to 10 Hz. 50% seated and 50% standing crowds = 0%, 5%, 10%, 20%, 30% and 40% m s F x Crowd mass = m s
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University of Oxford Dynamic analysis (2) DMF = Peak displacement / Static displacement SDOF structure Seated / standing crowd Displacement Excitation force Interaction force Acceleration +
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University of Oxford Results – DMF vs Frequency 2 Hz structure4 Hz structure
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University of Oxford Summary of results (1): Resonant frequency reduction factor F.R.F. = Change in frequency / Frequency of bare structure
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University of Oxford Summary of results (2): DMF reduction factor DMF R.F. = Change in DMF max / DMF max of bare structure
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University of Oxford Why reduced-DOF system? Full crowd-model: 2DOF crowd + SDOF structure A simplified model for Easier analysis Insight into the dynamics
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University of Oxford Equivalent SDOF system SDOF system transfer function: Curve-fit DMF frequency response curve over bandwidth
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University of Oxford Dynamic properties
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University of Oxford Error analysis (1) Peak DMF relative error Resonant frequency relative error
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University of Oxford Error analysis (2)
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University of Oxford Equivalent 2DOF system ms ms F x Crowd modelled as SDOF system Structure remains the same SDOF system
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University of Oxford SDOF crowd model
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University of Oxford Dynamic analysis SDOF structure SDOF Seated / standing crowd Displacement Excitation force Interaction force Acceleration +
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University of Oxford Error analysis
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University of Oxford Bode diagrams
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University of Oxford Conclusions Passive crowd adds significant damping 1 to 4 Hz – behaviour of a SDOF system > 4 Hz – behaviour of a 2DOF system
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