2008
DOI: 10.1016/j.trb.2007.08.004
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Explicit construction of entropy solutions for the Lighthill–Whitham–Richards traffic flow model with a piecewise quadratic flow–density relationship

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Cited by 28 publications
(36 citation statements)
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“…The first traffic flow test example is taken from [18]. The flow-density function is given by a concave function qðqÞ ¼ À0:4q 2 þ 100q; 0 6 q 6 50; À0:1q 2 þ 15q þ 3500; 50 6 q 6 100; À0:024q 2 À 5:2q þ 4760; 100 6 q 6 350:…”
Section: Distance (Km)mentioning
confidence: 99%
“…The first traffic flow test example is taken from [18]. The flow-density function is given by a concave function qðqÞ ¼ À0:4q 2 þ 100q; 0 6 q 6 50; À0:1q 2 þ 15q þ 3500; 50 6 q 6 100; À0:024q 2 À 5:2q þ 4760; 100 6 q 6 350:…”
Section: Distance (Km)mentioning
confidence: 99%
“…In this case k 0 = −11.6569 in (22)- (25). The exact solution of these problems can be worked out using the procedure in this paper, shown as solid lines in Figures 12 and 13, in comparison with the numerical solution obtained by the WENO scheme using N = 1000 uniform grid points, shown as circles.…”
Section: Example 2 (Rarefaction Waves)mentioning
confidence: 95%
“…As for each fixed ∆t, S(∆t) and S (∆t) can both be readily computed, we can easily set up a Newton iteration to solve for the root of S(∆t) with ∆t = 0 as the initial guess. We can follow the discussion in the appendix of Lu et al (2006) to discuss the uniqueness of the solution to equation (56) before the natural break time, thereby facilitating the convergence of the Newton iteration process.…”
Section: Solution Proceduresmentioning
confidence: 99%
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