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Predicting Human Induced Vibration with GSA Footfall. Today’s Team. Peter Debney Application Specialist. Nigel Rees Sales Manager. Today’s Team. Peter Debney Application Specialist. Rhys Lewis Consultant. GoToWebinar Attendee Interface. 1. Viewer Window. 2. Control Panel.
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Today’s Team Peter Debney Application Specialist Nigel Rees SalesManager
Today’s Team Peter Debney Application Specialist Rhys Lewis Consultant
GoToWebinar Attendee Interface 1. Viewer Window 2. Control Panel If you cannot hear, please check this setting Oasys Software : GSA Footfall
Agenda • Product Demonstration • GSA • Questions and Answers NB: this webinar is designed as an introduction to GSA and footfall and is designed to provide an overview.
Who is Oasys? • Wholly owned by Arup • Formed in 1976 to develop software for in-house and external use • Most developers are engineers who have moved to programming • In recent years have added marketing and sales staff • Since 2003 have expanded the development team worldwide • Wide network of resellers and channel partners
Structural Geotechnical Document Management Crowd simulation CAD Sustainability
Vibration The Problem
The effects of vibration • Structural Damage • Inelastic response – overload • Fatigue • Discomfort • Bouncy floors and stairs • Wind-induced sway of buildings • Ride comfort • Noise • Machine operation • Machine operability • High precision manufacturing facilities • Medical facilities • Laboratories
The effects of vibration • Structural Damage • Inelastic response – overload • Fatigue • Discomfort • Bouncy floors and stairs • Wind-induced sway of buildings • Ride comfort • Noise • Machine operation • Machine operability • High precision manufacturing facilities • Medical facilities • Laboratories
What is Footfall? Human induced vibration
What is Footfall? Vibration • A bridge as a simply supported beam • (b) The first mode of vibration • (c) The displacement of mid-span after someone jumps once at mid-span
What is Footfall? Vibration
What is Footfall? Vibration
Results Velocities and Accelerations f = 1 / T ω = 2 π f x = X sin ωt v = Xω cos ωt a = -Xω2 sin ωt
Results What is R? BS 6472 base curve for human perception
Modal mass F = ma a = F/m
Resonance 1st harmonic
Resonance 2nd harmonic
Resonance 3rd harmonic
Resonance 4th harmonic
resonance excitation too fast for any significant response 1 - static Resonance and Damping Dynamic amplification under harmonic (single frequency) loading
Resonance and Damping Dynamic amplification with multiple harmonics
Resonance and Damping Dynamic amplification with multiple harmonics
Footfall - Simple Method f0 = 18 / √δ
Webinar has now Ended • Contact Details • Peter Debney – peter.debney@arup.com • Nigel Rees – nigel.rees@arup.com • Next Webinars • August 15th: Raft and Soil-Structure Interaction • September 19th: Concrete Design