Understanding and Modeling Driver Behavior in Dense Traffic Flow

 

Principal Investigator:

H. Michael Zhang

Dept. of Civil and Environmental Engineering

University of California at Davis

Davis, CA 95616

Ph: 530-754-9203

Fax: (530)-752-7872

hmzhang@ucdavis.edu

 

Funded by a UCTC Year 13 grant.

 


 

 

This research will examine drivers’ car-following behavior in dense traffic flow and identify the critical behavioral elements and parameters that control traffic flow phase transitions.  Such an understanding will aid the development of more sound microscopic traffic models that are the central building blocks of popular traffic simulation packages such as CORSIM, TRANSIMS and PARAMICS.  The main task of this research concerns the development of a car-following model that reproduce the capacity gap and hysteresis observed in traffic flow.

 

Regardless of the cause of congestion, congested traffic usually exhibits two prominent features: 1) an initial front that induces sharp flow/density/speed changes, and 2) a prolonged period of stop-and-go motion across the congested region after the front passes.   Viewed in the phase plane, these features translate into flow-density or speed-density or flow-speed jumps near a critical density/speed/flow region and periodic orbits, or hysteresis loops,  in the high density or low speed region. Eddie  (1961) from Lincoln Tunnel data, first noticed the existence of jumps in the density-speed scatter plot and hypothesized that speed-density or flow-density phase plots have two disjoint branches––one for free-flow traffic and the other for congested traffic, with the maximum flow of free-flow branch considerably higher than that of the congested branch, hence the name ``capacity drop''.  Eddie noted that this jump in flow/speed could be an intrinsic property of vehicular traffic flow.  Drake,  Schofer and May  (1967)  applied the two-regime hypothesis to traffic data and found that it produced the  best fit with lowest standard error.  Other experimental evidence of the existence of the ``capacity drop''  is from Japanese and German highways.  Koshi, Iwasaki, and Ohkura (1983) analyzed traffic data from the Tokyo Expressway and found that their flow-density plots resembles the mirror image of a reversed  lambda,  with data points scattered more widely near the right  leg of the reversed lambda. Kerner and Rehborn  (1998), on the other hand, have shown that in German data the flow rate out of a wide jam is considerably lower than the maximal possible flow rate in free flow and a multitude of homogeneous states of synchronized flow covers a broad region around the characteristic line J. The first clear experimental evidence of traffic hysteresis was provided by Treiterer and Myers (1974). These authors studied a  platoon of vehicles and estimated their average flow, density and travel speed. They found that both the flow-density and speed-density plots have loop structures. Other experimental evidence of traffic hysteresis include the observations of Maes (1979) on Belgian  highways and Zhang  (1999) on California highways.  Zhang  (1999) also  noted the linkage between hysteresis and stop-start waves and provided a traffic theory to model it. The first exploitation of traffic hysteresis, however,  is by Newell  (1965), who hypothesized that drivers respond to stimulus differently in acceleration and deceleration and developed a model that contains hysteresis loops. Newell's hypothesis on driver behavior was corroborated by experimental observations of Forbes (1963), who observed that a sudden change in drivers' response time occurs before and after a sudden deceleration. Forbes further suggested that this sudden change of response time explains the jumps found on various phase diagrams and proposed flow-density diagrams with multiple branches.

Conventional traffic stream models (i.e., flow-density or speed-density diagrams or formulas), however, are usually described by continuous or even smooth functions that contain neither jumps nor hysteresis loops.  A common property of these models is that most of these functions can be derived from one car-following model or another under steady-state traffic conditions, which provides them a behavioral and theoretical foundation. The fact that these car-following models lead to smooth flow-density or speed-density relations attest, to a certain degree, their inadequacy to model complex traffic flow patterns that exhibit capacity drops and hysteresis loops. This is not surprising if one considers that conventional car-following models treat both drivers and roads as homogeneous entities---that is, they are modeling identical drivers who travel on homogeneous roads.  The traffic that produces capacity drops and hysteresis loops, on the other hand, comprise diverse groups of drivers who travel on inhomogeneous roads and may behave differently under different driving conditions. A plausible car-following theory that explains these nonlinear phenomena must consider these inhomogeneities.

 

This research proposes a car-following model that captures situation-dependent driving behavior. A central concept in this model is that the time gap a driver adopts depends on both the driving condition and the type of motion (acceleration, deceleration, or coasting) he is in:

                                                                                                   (1)

where is the time gap adopted by driver n at time t ,  is the space gap between driver n’s vehicle and the immediate vehicle ahead of him, and P(t) indicates the type of motion the driver is in at time t.  Fig.1 shows the definition of variables.

 

Figure 1.  Definitions of time and space gaps

 

From the definitions of time and space gaps, we have the following car-following

model

 

                                                                                                    (2)

 

where  is the travel speed of driver n’s vehicle at time t.  

 

From Eq. 2 we can see that driver behavior is embodied in the time gap variable, which is a function of traffic condition (captured by space gap, a measure of crowdness) and motion type (acceleration/deceleration/coasting).   By specifying different forms for the function H, we obtain various  specific car-following models, among which some were discussed earlier in the text and some are brand new models that can reproduce either the capacity drop or traffic hysteresis or both phenomena.  The form of the function H can be depicted graphically, and Figs 2 and 3 show two specifications of the H function, which lead to two specific cases of the car-following model, which we shall refer as Model C and Model D respectively.  The corresponding fundamental diagrams for steady-state traffic for Models C and D are also shown in Figs 2 and 3 on the right, and as can be seen from these figures, capacity drop and hysteresis are built into the behavior of these models. Indeed this can be verified through traffic simulation, which shows the dynamic evolution of traffic governed by the proposed car-following model.  These results are shown in Figs 4 and 5, respectively.  The capacity drop and hysteresis are evident in these figures (the details of the theoretical and numerical analysis of these models can be found in Zhang and Kim , 2001).  

 

In summary, both theoretical analysis and numerical simulations have demonstrated the potential of the new car-following model to describe complex traffic flow phenomena. Further research will be devoted to validate this model with experimental data. It is hoped that this new model, once validated, can provide a more realistic and powerful traffic flow model for high fidelity microscopic traffic simulations.

 

Papers:

Zhang, H. Michael, and T. Kim, "A Car-Following Theory for Multiphase Vehicular Traffic Flow," Transportation Research Board.

Zhang, H. Michael, and T. Kim, "Understanding and Modeling Driver Behavior in Dense Traffic Flow," working paper, October 10, 2002.

References:

Drake, J.S., Schofer, J.L., and May, A.D.,(1967). A Statistical Analysis of Speed Density Hypothesis. Highway Research Record 154,  pp. 53-87.

 

Edie, L. C. (1961). Following and Steady-State Theory  for Non-congested Traffic, Operations Research, Vol .9, pp.66-76.

 

Forbes, T.W. (1963). Human Factor Considerations in  Traffic Flow Theory. Highway research Board, Record 15, pp. 60-66.

 

Kerner, B.S. (1998) Experimental features of self-organization in traffic flow, Physical Review Letters Vol. 81, No. 17,  pp.3797-3800.

 

Koshi, M., Iwasaki, M., Ohkura, I. (1983). Some Findings  and an Overview on Vehicular Flow Characteristics,  Proc. 8th  Intl. Symp. On Transportation and Traffic Flow Theory (V. Hurdle, E. Hauer, G. Stuart ed.) pp. 403-426.

 

Maes, W. (1979) Traffic data collection system for the Belgian motorway

Network–measures of effectiveness aspects.  Proceedings of the International Symposium on Traffic Control Systems, Vol. 2D–Analysis and Evaluation, pp. 45--73.

 

Newell, G.F.(1961).  Nonlinear Effects in the  Dynamics of Car Following,  Operations Research, Vol 9,  209-229.

 

Treiterer, J. and Myers, J.A. (1974). The Hysteresis Phenomenon in Traffic Flow. Proc. 6th Intl. Symp. on Transportation and Traffic theory, (D.J. Buckley ed.), pp. 13-38.

 

Zhang H. M. and T. W. Kim (2001) A car-following theory for multiphase vehicular traffic flow, pre-print 01-3456, 2001TRB Annual Meeting.

 

Zhang, H.M.(1999). A mathematical theory of traffic hysteresis, Transportation Research, Part B 33,  1-23.

 

 

 

 

 

 

 

Figure 2 The H function and the corresponding fundamental diagram for Model C

 

 

Figure 3 The H function and the corresponding fundamental diagram for Model D

 

Figure 4 Simulation results for Model C on a ring road

 

 

Figure 5 Simulation results for Model D on a ring road