Some exact solutions to the Lighthill-Whitham-Richards-Payne traffic flow equations (Q2854118)
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scientific article; zbMATH DE number 6216146
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Some exact solutions to the Lighthill-Whitham-Richards-Payne traffic flow equations |
scientific article; zbMATH DE number 6216146 |
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17 October 2013
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traffic flow
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exact solution
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Lambert-W function
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Lagrangian coordinates
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Some exact solutions to the Lighthill-Whitham-Richards-Payne traffic flow equations (English)
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The authors study the Lighthill-Whitham-Richards-Payne (LWRP) traffic flow equations given by the system of partial differential equations NEWLINE\[NEWLINE \rho_t + u \rho_x = - \rho u_x, NEWLINE\]NEWLINE NEWLINE\[NEWLINE u_t + u u_x = (V(\rho)- u))/\tau_0 - (\nu_0/\rho) \rho_x. NEWLINE\]NEWLINE They introduce Lagrangian coordinates to eliminate certain nonlinearities.NEWLINENEWLINEFor exponential profiles of the initial fluid densities of the form NEWLINE\[NEWLINE \rho_0(x) = a \exp(\pm \lambda \xi), NEWLINE\]NEWLINE they find an explicit expression for the fluid density \(\rho\) in terms of \(X\) and \(t\). In this representation, the Lambert W-function appears.NEWLINENEWLINETo obtain the solution, the system is transformed to a nonlinear second-order equation that can be factorized as a product of two first-order operators similar to the wave equation.
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