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F - 5th International Conference on Sustainable Construction and ...

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Day of Research 2010 – February 10 – Labo Soete, Ghent University, Belgium<br />

With appropriate initial c<strong>on</strong>diti<strong>on</strong>s at t=0, soluti<strong>on</strong> of U at different time steps can be found, using<br />

Equati<strong>on</strong>s (17), (20) <strong>and</strong> (21). As the time step becomes smaller, the numerical soluti<strong>on</strong> c<strong>on</strong>verges to the<br />

exact soluti<strong>on</strong>. An example of a FE transient dynamics analysis is shown in Figure 12, where a footbridge,<br />

Wilcott bridge, is excited using a walking pedestrian [21]. The Wilcott footbridge is a newly c<strong>on</strong>structed FRP<br />

composite footbridge crossing the new A5 Nesscliffe Bypass near Shrewsbury, UK. Wilcott footbridge is a<br />

suspensi<strong>on</strong> bridge, has a single span of 50.24 m <strong>and</strong> provides a footway of 2.3 m wide. The finite element<br />

package ANSYS was used to simulate the transient dynamics resp<strong>on</strong>se of the footbridge. 3-D beam<br />

elements (Figure 12(a)) were used to model all the structural members including; cross beams, deck, posts,<br />

cables <strong>and</strong> hangers. Mass elements were used to model h<strong>and</strong>rails, ballast in the cells, <strong>and</strong> deck finishing. A<br />

time history analysis is performed to calculate the dynamic resp<strong>on</strong>se of the footbridge under the acti<strong>on</strong> of a<br />

walking pedestrian at a frequency close to the sec<strong>on</strong>d vertical natural frequency of the bridge (1.6 Hz).<br />

Humans walking pacing rate normally lies in the range 1.6-2.4Hz. The vertical dynamic load induced <strong>on</strong> the<br />

footbridge by a pedestrian taken from BS5400 is a pulsating moving load of: F(t)=180sin(ω.t) N. The<br />

displacement time resp<strong>on</strong>se in the mid-span of the bridge is shown in Figure 12(b).<br />

u (cm)<br />

(a)<br />

Figurer 12. Wilcott bridge: (a) FE model <strong>and</strong> (b) Mid-span resp<strong>on</strong>se due to a walking pedestrian<br />

(b)<br />

10 TRAFFIC FLOW ANALYSIS<br />

In traffic flow analysis, the degree of freedom is the traffic density. The governing partial differential<br />

equati<strong>on</strong> of traffic flow is known by LWR (Lighthill, Witham <strong>and</strong> Richards) model. For <strong>on</strong>e dimensi<strong>on</strong>al<br />

c<strong>on</strong>stant speed traffic flow, LWR equati<strong>on</strong> is given by [22]:<br />

k<br />

u<br />

t<br />

k<br />

0<br />

x<br />

o<br />

(22)<br />

Where k is the traffic density (vehicle/m), which is a functi<strong>on</strong> of time <strong>and</strong> space, <strong>and</strong> uo<br />

is the traffic speed<br />

(m/s). Applying variati<strong>on</strong>al formulati<strong>on</strong> or Galerkin method to Equati<strong>on</strong> (22), the FE equati<strong>on</strong> in matrix form<br />

is obtained as:<br />

k<br />

<br />

<br />

t<br />

<br />

<br />

B k<br />

0<br />

A (23)<br />

Again, the soluti<strong>on</strong> of Equati<strong>on</strong> (23) is obtained in different time steps using numerical integrati<strong>on</strong>. An<br />

example of traffic flow analysis is a simulati<strong>on</strong> of a 5 km road [22], where the boundary c<strong>on</strong>diti<strong>on</strong>s at the<br />

beginning of the road (x=0) are as shown in Figure 13(a). The c<strong>on</strong>vergence of traffic flow density at a<br />

distance of 2 km is plotted in Figure 13(b) by c<strong>on</strong>sidering different element sizes (Δx).<br />

(a)<br />

(b)<br />

Figurer 13. FE traffic flow analysis: (a) Boundary c<strong>on</strong>diti<strong>on</strong>s at the beginning of the road x=0 <strong>and</strong> (b)<br />

C<strong>on</strong>vergence of density at x= 2 km as functi<strong>on</strong> of Δx<br />

38 Copyright © 2010 by Labo Soete

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