So first of all, I would like to thank the organizing committee and the scientific committee
for inviting me here.
So I'm definitely a PDE person and when thinking about what to propose as a talk here, I thought
that the most suitable subject was the work of one of my former PhD students, Alexandra
Wurz, which is by the way now in the Fraunhofer in Kaiserslautern, and which I co-advised
with my colleague, Michele Bignois, which is an expert in statistical optimization.
So the work focuses on the calibration of microscopic traffic flow models.
So these models basically are meant to describe the spatiotemporal evolution of some aggregate
quantities like the mean traffic density, rho, which is roughly speaking the number
of vehicles per unit space.
Then we can consider the mean velocity V, which is the average distance covered by the
vehicles per unit time, and the traffic flow, which is the product of the two and gives
the number of vehicles per unit time.
This quantity can be measured on the road and the more traditional data sources are
magnetic loop detectors, which counts the vehicle passing at fixed positions on the
road.
And you can notice sometimes the traces on the pavement.
Nowadays there are many more sources of data which are in principle available, like video
recordings, flotist car data, and other sources, but for this work we consider magnetic loop
detectors, so traditional counting at fixed positions.
So to give you an idea of how this data looks like, this is an example taken from the highway
network close to Marseille that was provided by DIRMED, which is the public administrator
of this sector.
And these are the raw data, so not treated data, which basically mark the time at which
a vehicle crosses a given loop detector.
So here you have the ID of the loop.
Here you have its position given by the distance from some milestone.
Here is the day, the date, and the hour, the lane.
And then, so for this type of loop detectors, which are double, we also can retry the speed
at which the vehicle passes through.
And its length, we want to distinguish which type of vehicle is it.
There are also other sensor types that are single loop detectors that cannot measure
the speed, but instead can measure the occupancy, which is basically the ratio of time the loop
is occupied by a vehicle, and this is somehow proportional to the density of the vehicle.
So from this, we have a direct measure of the flow, a measure either of the density
or of the speed, and we can retry the third component, either the density and the speed,
by considering this formula here.
So moving to the modeling, the basic assumption of microscopy model is the mass conservation.
So we start from a conservation equation of this form, so it's a partial differential
equation, which says that the partial derivative of the density plus the partial derivative
of the flux is equal to zero.
So to close the model, one of the first suggestions was given by Lighting-Gridham and Richard,
and was to associate to each density value a given speed value, so to write the speed
as a function of the density.
So the basic assumption is that the speed must be decreasing with density or increasing
with density, and corresponding fundamental diagram, which is the product of the density
and the speed, is usually a concave down function.
So this is the most simple traffic flow model, microscopy traffic flow model you can deal
with, and it's referred to as a first order traffic flow model.
Nevertheless, when you look at data and how they look like if you plot a speed density
Presenters
Dr. Paola Goatin
Zugänglich über
Offener Zugang
Dauer
00:28:01 Min
Aufnahmedatum
2025-04-28
Hochgeladen am
2025-04-29 15:45:47
Sprache
en-US
• Alessandro Coclite. Politecnico di Bari
• Fariba Fahroo. Air Force Office of Scientific Research
• Giovanni Fantuzzi. FAU MoD/DCN-AvH, Friedrich-Alexander-Universität Erlangen-Nürnberg
• Borjan Geshkovski. Inria, Sorbonne Université
• Paola Goatin. Inria, Sophia-Antipolis
• Shi Jin. SJTU, Shanghai Jiao Tong University
• Alexander Keimer. Universität Rostock
• Felix J. Knutson. Air Force Office of Scientific Research
• Anne Koelewijn. FAU MoD, Friedrich-Alexander-Universität Erlangen-Nürnberg
• Günter Leugering. FAU, Friedrich-Alexander-Universität Erlangen-Nürnberg
• Lorenzo Liverani. FAU, Friedrich-Alexander-Universität Erlangen-Nürnberg
• Camilla Nobili. University of Surrey
• Gianluca Orlando. Politecnico di Bari
• Michele Palladino. Università degli Studi dell’Aquila
• Gabriel Peyré. CNRS, ENS-PSL
• Alessio Porretta. Università di Roma Tor Vergata
• Francesco Regazzoni. Politecnico di Milano
• Domènec Ruiz-Balet. Université Paris Dauphine
• Daniel Tenbrinck. FAU, Friedrich-Alexander-Universität Erlangen-Nürnberg
• Daniela Tonon. Università di Padova
• Juncheng Wei. Chinese University of Hong Kong
• Yaoyu Zhang. Shanghai Jiao Tong University
• Wei Zhu. Georgia Institute of Technology