Microscopic theory of spatial-temporal congested traffic patterns at highway bottlenecks

Physical Review E - Statistical, Nonlinear, and Soft Matter Physics

Volumn 68, Issue 3 2, 2003, Pages 361301-3613020

  Kerner, Boris S ^a   Klenov, Sergey L ^b  

^a DAIMLER AG   (Germany)

^b MOSCOW INSTITUTE OF PHYSICS AND TECHNOLOGY   (Russian Federation)

Author keywords

[No Author keywords available]

Indexed keywords

FLOW PATTERNS; PHASE TRANSITIONS; SYNCHRONIZATION; VEHICLES;

HIGHWAY BOTTLENECKS; TRAFFIC PATTERNS;

HIGHWAY TRAFFIC CONTROL;

EID: 0242579537     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: None     Document Type: Article

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54. n/10), the other model parameters are the same as in Sec. II C except λ = 0.5. Model (1)-(8) is a generalization of KKW cellular automata model [28] for the continuous speed.
55. th≪1.
56. Different 2D states of synchronized flow are related to different critical perturbation amplitudes. It could be expected that there should be also infinite number of different critical branches for the S → J transition. The critical branches in Fig. 4 are an averaging of these different critical branches.
57. out
58. (B) is shown by the curve 3′ in Fig. 4(e)].
59. Also in Ref. [12] in MSP which is far away of the bottleneck a wide moving jam can emerge. This effect occurs when model parameters are slightly different from those used for simulations (Sec. II C).
60. An example of ASP is shown in Fig. 17(c).