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ra_forever8
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On a stretch ofsingle-lane road with no entrances or exits the traffic density r(x,t)is a continuous function of distance xand time t, for all t > 0, and the traffic velocity u(r) is a function of density alone.
Two alternative models are proposed to represent u:
(i) u= uSL (1 – r^n/ r^nmax)
where n is a positive constant
(ii) u= 1/3 uSL In (rmax/r)where uSLis the maximum speed limit on the road and rmax is themaximum density of traffic possible on the road (corresponding tobumper-to-bumper traffic).
a) Evaluate the maximum rate of traffic flow for cases (i)and (ii) above. Show that for both cases the maximum rate of traffic flow isless than uSLrmax and that for case (i)it increases towards this upper limit as nbecomes very large.
b) It is assumed that a model of the form given in case (i)is a reasonable representation of actual traffic behaviour. Apply the method ofcharacteristics to analyse the following situation. A queue of cars is stoppedat a red traffic light on a road for which the maximum speed limit is 40 m.p.h.It may be assumed that the queue is very long and that the road ahead of thelight is empty of traffic. The light turns green and remains green for only 45seconds. If a car which is initially a quarter of a mile behind the light getsthrough before the light changes back to red determine the smallest integervalue that n can have. (Hint: showinitially that the car will not start moving until a certain time after thelight has turned green, and then solve the appropriate differential equationfor the position of the car.)
=> The attempt at a solution
For part (a) you need to observe that the flow rate f(x,t) in vehicles per unit time is u(x,t)ρ(x,t) .
Mow,to show (i) and (ii) that u(x,t)≤u sl , then as ρ(x,t)≤ρ max I will have shown that the flow rate: f(x,t)≤u sl ρ max .
b)Consider a road element between x and x+Δx the traffic flow into the element at x per unit time is u(ρ(x,t))ρ(x,t) and out at x+Δx is u(ρ(x+Δx,t))ρ(x+Δx,t) Therefore the rate of change of car numbers in the element is:
∂N ∂t =u(ρ(x,t))ρ(x,t)−u(ρ(x+Δx,t))ρ(x+Δx,t)
and so the rate of change of density in the element is:
1 Δx ∂N ∂t =u(ρ(x,t))ρ(x,t)−u(ρ(x+Δx,t))ρ(x+Δx,t) Δx
Now take the limit as Δx→0 to get:
∂ρ ∂t =∂ ∂x u(ρ)ρ
(Could please confirm with my answer, I am not sure and unable to move on from there. Please help me)
Two alternative models are proposed to represent u:
(i) u= uSL (1 – r^n/ r^nmax)
where n is a positive constant
(ii) u= 1/3 uSL In (rmax/r)where uSLis the maximum speed limit on the road and rmax is themaximum density of traffic possible on the road (corresponding tobumper-to-bumper traffic).
a) Evaluate the maximum rate of traffic flow for cases (i)and (ii) above. Show that for both cases the maximum rate of traffic flow isless than uSLrmax and that for case (i)it increases towards this upper limit as nbecomes very large.
b) It is assumed that a model of the form given in case (i)is a reasonable representation of actual traffic behaviour. Apply the method ofcharacteristics to analyse the following situation. A queue of cars is stoppedat a red traffic light on a road for which the maximum speed limit is 40 m.p.h.It may be assumed that the queue is very long and that the road ahead of thelight is empty of traffic. The light turns green and remains green for only 45seconds. If a car which is initially a quarter of a mile behind the light getsthrough before the light changes back to red determine the smallest integervalue that n can have. (Hint: showinitially that the car will not start moving until a certain time after thelight has turned green, and then solve the appropriate differential equationfor the position of the car.)
=> The attempt at a solution
For part (a) you need to observe that the flow rate f(x,t) in vehicles per unit time is u(x,t)ρ(x,t) .
Mow,to show (i) and (ii) that u(x,t)≤u sl , then as ρ(x,t)≤ρ max I will have shown that the flow rate: f(x,t)≤u sl ρ max .
b)Consider a road element between x and x+Δx the traffic flow into the element at x per unit time is u(ρ(x,t))ρ(x,t) and out at x+Δx is u(ρ(x+Δx,t))ρ(x+Δx,t) Therefore the rate of change of car numbers in the element is:
∂N ∂t =u(ρ(x,t))ρ(x,t)−u(ρ(x+Δx,t))ρ(x+Δx,t)
and so the rate of change of density in the element is:
1 Δx ∂N ∂t =u(ρ(x,t))ρ(x,t)−u(ρ(x+Δx,t))ρ(x+Δx,t) Δx
Now take the limit as Δx→0 to get:
∂ρ ∂t =∂ ∂x u(ρ)ρ
(Could please confirm with my answer, I am not sure and unable to move on from there. Please help me)