Title: 3Phase theory introduction
13Phase theory introduction
Peter Los Frank Zuurbier Huizhao Tu
TRAIL Course The Physics of Traffic
2DEFINITIONS
- Traffic variables e.g. flow (q), (vehicle) speed
(v), time/space gap (g), density (?) - Traffic (control) parameters e.g. weather, road
conditions (alignment, width, etc) vehicle
characteristics - Traffic state A state characterized by certain
set of variables and parameters - Traffic phase set of traffic states in with a
specific (unique) spatiotemporal features
3DEFINITIONS
UPstream backwards
DOWNstream forward
IN flow
OFF flow
OUT flow
ON flow
4DEFINITIONS
- FRONT
- a region where a spatial transition is performed
between different traffic - a) states
- b) phases
- Downstream front edge of the state forwards the
direction of traffic flow - Upstream front edge of the state backwards the
direction of traffic flow
5DEFINITIONS
direction of traffic flow
Variable (speed, flow, etc)
distance
upstream front
downstream front
state UP
state IN
state DOWN
6MEASUREMENTLocal traffic variables
- by double induction loops we measure variables
- ?ti length of pulse (and pause)
- ?ti time lag between 2 loops
- ? vi , di speed length of vehicle
- ? ? , g time and distance gap
- ? macroscopic traffic flow
- q, ? and v (temporal) speed of flow???
7MEASUREMENT
- at bottlenecks(control parameters change)
- to be able observe the spatiotemporal changes
8FUNDAMENTAL DIAGRAMempirical observations
9FUNDAMENTAL DIAGRAMModels
- (Deterministic) Macroscopic
- L-W-R (1955-56), Prirogine (1959)Payne (1971)
and further developments - (Deterministic) Microscopiccar following
acceleration gap - optimal velocity accel. gap speed
difference - inteligent driver accel. speed gap ?
speed - Stochastic
- Gipps (1981) safe distance
- cellular automata
10FUNDAMENTAL DIAGRAMShock-wave theory
- Conservation of number of vehicles
- based on the particle conservation law
- Shock-wave formula ?1(v1-vp) ?2(v2-vp)
- Velocity of the shock-wave
11FUNDAMENTAL DIAGRAM LWR model
- Lighthill Whitham (1955) and Richards (1956)
- the flow (q) is a function of the density (?)
- qq(?) i.e. only one independent variable
- Conservation balance formula
- solution Kinematic waves
12PROBLEMS OF FD APPROACH
- it works only in homogeneous steady-states
- i.e. same distances, same time-dependent speed
- describes the free-flow well-enough
- at higher density presents only averaged
characteristics of congested patterns(not
considering noise and perturbations)
13FUNDAMENTAL DIAGRAM 2-phase theory
- Prirogine and Herman (1971)
- concept of collective flow in FD-aproach
- 2-phase traffic flow theory
- - free flow and
- - collective flow at higher densities
- synchronization of vehicle speed (probability of
passing is a monotonous decreasing function of
density)
14FUNDAMENTAL DIAGRAM Moving jams scenarios
- Herman et al. and KomentaniSasaki (1958-59)
- ideas of statistical physics to explain the
moving jams - instabilities (driver behaviour
over-decelaration) - critical point (density)
- KernerKornhauser (1994)
- Metastable traffic flow - below the critical
density
15WIDE MOVING JAM
direction of traffic flow
Variable (speed, flow, etc)
distance
upstream front
downstream front
state UP
state IN
state DOWN
- WMJ width of state in gtgt width of fronts
16FUNDAMENTAL DIAGRAMMoving jam characteristics
- J-line determined by characteristics of free
flow by accelerating from the standstill - independent parameters(only if free
outflow!)?del , qout , ?min , vmax - point j is the treshold of metastability
qmax
j
unstable
qout
J - slope vg
stablefree flow
?min
?max
17FUNDAMENTAL DIAGRAM Metastability of free flow
- line K
- vup lt vg
- the width of jam decreases
- line N
- vup gt vg
- .the width of jam increases
n ?n qn
qmax
qout
N
K
?min
?max