Pedestrian Dynamics: Feedback Control of Crowd Evacuation - download pdf or read online

By Pushkin Kachroo

Powerful evacuations can retailer lives. This ebook presents mathematical types of pedestrian hobbies that may be used particularly for designing suggestions regulate legislation for powerful evacuation. The publication additionally presents a variety of suggestions keep an eye on legislation to complete the powerful evacuation. It publication makes use of the hydrodynamic hyperbolic PDE macroscopic pedestrian versions considering the fact that they're amenable to suggestions keep watch over layout. The regulate designs are acquired via diversified nonlinear options.

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This example can U0 ( x) Um Um / 2 xk x t x Fig. 8. 6 Method of Characteristics 27 U0 ( x) Um Um / 2 xk x t ? x Fig. 9. Characteristics do not specify solution in the wedge be related to conditions of a red light turns to green. As we all observe in real situation, cars start to accelerate from high density (low speed) to low density (higher speed). The exact solution for this data shows that there is a region untouched by any characteristics from the given initial data. Thus, the method of characteristics did not identify a solution in this region.

57) is the sound wave speed. 49) from its microscopic counterpart. 5 Traffic Flow Model 1-D 21 The conservative form of this model is derived next. 58) then expand the conservation of mass equation ρt + ρvx + vρx = 0. 61) or in lagrangian form as (v − V (ρ))t + v (v − V (ρ))x = 0. 64) to get (ρ(v − V (ρ)))t − ρt (v − V (ρ))+ (ρv (v − V (ρ)))x − (vρ)x (v − V (ρ)) = 0. 66) where our states are given by ρ and ρ(v − V (ρ)). 32), such that ⎡ ⎤ X + ρV (ρ) ρ ⎦. 67) Q= , F (Q) = ⎣ X 2 X − XV (ρ) ρ 22 2 Traffic Flow Theory for 1-D The Jacobian is then can be found to be ⎡ V (ρ) + ρV (ρ) ∂F ⎣ X2 A(Q) = = − − XV (ρ) ∂Q ρ2 1 2X + V (ρ) ρ ⎤ ⎦.

This model uses two-coupled PDE’s to describe crowd flow; the conservation of continuity and a second equation that looks like the momentum equation in fluid flow with a modification to the “pressure” term to mimic crowd motion. This model is known for its isotropic nature that is preserved when we extend the model to 2-D space assuming pedestrian motion is influenced from all directions. 24) from 1-D to 2-D, and add relaxation terms to allow bi-directional flow. 10) where the density ρ(x, y, t) depends on the two spatial dimensions and time, v(x, y, t) and u(x, y, t) are the x-axis and y-axis components of the velocity.

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