A highway contains a uniform distribution of cars moving at maximum flux in the $x$-direction, which is unbounded in $x$. Measurements show that the car velocity $v$ obeys the relation: $v = 1 − ρ$, where ρ is the number of cars per unit length. An on-ramp is built into the highway in the region $0 ≤ x < 1$. Town planners want to understand whether they should limit the rate per unit length of cars, $α$, entering the highway via this on-ramp, to avoid traffic jams on the highway. The on-ramp is closed for all time $t < 0$, and opens for $t ≥ 0$.
Identify the presence of all key features of the problem, including any fans/shocks.
Hi, can someone please explain to me how to do such a question? I'm struggling to understand this conceptually, the process of identifying fans and shocks, what exactly I'm supposed to be looking for. Any help would be appreciated, thanks in advance.
The macroscopic traffic-flow model by Lighthill-Whitham-Richards (LWR) is an hydrodynamic model for traffic flow on a single infinite road. It consists in a scalar hyperbolic conservation law, which represents the conservation of cars (continuity equation): $$ \frac{\partial}{\partial t}\rho + \frac{\partial}{\partial x}Q (\rho) = 0 \, , $$ where the flux $Q(\rho) = \rho\, v(\rho)$ depends only on the density of cars $\rho$. The simplest expression for the car velocity $v(\rho)$, introduced by Greenshields, reads $$ v(\rho) = v_\max \left(1 - \frac{\rho}{\rho_\max}\right) . $$ Therefore, the present case corresponds to $v_\max = 1$ m/s and $\rho_\max=1$ car/m. The flux function $Q (\rho) = \rho \left(1- \rho\right)$ is maximum at $\rho = 1/2$ car/m, which is assumed to be the uniform density of cars at negative times. The characteristic curves such that $\rho(x,t)=\rho(x(t),t)$ satisfy $$ \frac{d\rho}{dt} = \frac{\partial\rho}{\partial t} + \underbrace{\frac{dx}{dt}}_{Q'(\rho)} \frac{\partial\rho}{\partial x} = \alpha \boldsymbol{1}_{0\leq x(t) < 1,\, t\geq 0} \, , $$ where $\alpha$ is the rate per unit length of cars entering the highway via an on-ramp. Several cases are considered:
A more quantitative solution is possible. At this point, one can decide to solve the conservation law with source term $$ \frac{\partial}{\partial t}\rho + \frac{\partial}{\partial x}Q (\rho) = \alpha \boldsymbol{1}_{0\leq x < 1,\, t\geq 0} $$ numerically, or to have a look at this post.