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Jorge A. Laval Workshop: Mathematical Foundations of Traffic IPAM, September 2015 1.

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Presentation on theme: "Jorge A. Laval Workshop: Mathematical Foundations of Traffic IPAM, September 2015 1."— Presentation transcript:

1 Jorge A. Laval Workshop: Mathematical Foundations of Traffic IPAM, September 2015 1

2 2 Multilane instabilities – FD scatter

3 3 3 Introduction: NGSIM US-101

4 4 Measurement method

5 5

6 6 Timid and aggressive behaviors Laval and Leclercq, Phil. Trans. Royal Society A, 2010.

7 7 Today’s hypothesis the random error in drivers acceleration processes may be responsible for most traffic instabilities: –Formation and propagation of oscillations –Oscillations growth –Hysteresis Laval, Toth, and Zhou (2015), A parsimonious model for the formation of oscillations in car-following models. Transportation Research Part B 70, 228- 238.

8 8 Outline stochastic desired acceleration model –for a single unconstrained vehicle plugin to Newell’s car-following model –upgrade simulation experiment –car-following experiment

9 9 Scope Car-following only, no lane changes Single lane Homogeneous drivers, no trucks

10 10 Stochastic desired accelerations Data collected with android app Platoon leader accelerating at traffic lights; i.e., an unconstrained vehicle

11 11 Stochastic desired accelerations desired acceleration  vehicle downstream does not constrain the motion

12 12 The SODE

13 13 Solution of the SODE Speed and position are Normally distributed:

14 14 Dimensionless formulation

15 15 An example acceleration process datamodel

16 16 Coefficient of Variation /  2 Parameter-free most variability at the beginning and for low speeds

17 17 Outline stochastic desired acceleration model –for a single unconstrained vehicle plugin to Newell’s car-following model –upgrade simulation experiment –car-following experiment

18 18 Plugin to Newell’s car-following model

19 19 The upgrade simulation experiment Single lane, 100m-100G% upgrade

20 20

21 21 Model captures oscillation growth

22 22 Model captures hysteresis Trajectory Explorer (trafficlab.ce.gatech.edu)

23 23 Model captures “concavity” Tian et al, Trans. Res. B (2015) Jian et al, PloS one (2014)

24 24 The upgrade simulation experiment cont’d: analysis of oscillations

25 25 Fourier spectrum analysis period = 3.3 min amplitude = 21.5 km/hr

26 26 Oscillations period and amplitude Large variance PDF not symmetric

27 27 Average speed at the botlleneck

28 28 Oscillations period and amplitude

29 29 Outline stochastic desired acceleration model –for a single unconstrained vehicle plugin to Newell’s car-following model –upgrade simulation experiment –car-following experiment

30 30 Car-following experiment 6-vehicle platoon, unobstructed leader 5Hz GPS devices and Android app in each vehicle two-lane urban streets around Georgia Tech campus Objective: –compare 6 th trajectory with model prediction –given: leader trajectory and grade G=G( x )

31 31 Car-following experiment

32 32 Example data

33 33 Trailing vehicle speed peak

34 34 Trailing vehicle speed peak: oblique trajectories

35 35 Trailing vehicle speed peak: oblique trajectories

36 36 Car-following experiment #1

37 37 Car-following experiment #2

38 38 Car-following exp. #2–Social force model

39 39 Car-following experiment #3

40 40 Car-following experiment

41 41 Q & A 41 THANK YOU !

42 42 90%-probability interval

43 43 Car-following experiment

44 44 Trajectory Explorer www.trafficlab.ce.gatech.edu

45 45 Source: NGSIM (2006) Models that predict Oscillations Unstable car-following models 2 nd -order models Delayed ODE type: oscillation period predicted ~ a few seconds (Kometani and Sasaki, 1958, Newell, 1961) ODE type, a few minutes (Wilson, 2008) Fully Stochastic Models Random perturbations not connected with driver behavior (NaSch, 1992, Barlovic et al., 1998, 2002, Del Castillo, 2001 and Kim and Zhang, 2008) Behavioral models Human error (Yeo and Skabardonis, 2009) Heterogeneous behavior in congestion (Laval and Leclercq, 2010, Chen et al, 2012a,b)

46 46 Parameter-free representation

47 47


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