Vanishing viscosity solutions of Riemann problems for models of polymer flooding

Author(s):  
Graziano Guerra ◽  
Wen Shen
2019 ◽  
Vol 266 (1) ◽  
pp. 312-351 ◽  
Author(s):  
Alberto Bressan ◽  
Graziano Guerra ◽  
Wen Shen

2021 ◽  
Vol 0 (0) ◽  
pp. 0
Author(s):  
John D. Towers

<p style='text-indent:20px;'>In [Andreianov, Coclite, Donadello, Discrete Contin. Dyn. Syst. A, 2017], a finite volume scheme was introduced for computing vanishing viscosity solutions on a single-junction network, and convergence to the vanishing viscosity solution was proven. This problem models <inline-formula><tex-math id="M1">\begin{document}$ m $\end{document}</tex-math></inline-formula> incoming and <inline-formula><tex-math id="M2">\begin{document}$ n $\end{document}</tex-math></inline-formula> outgoing roads that meet at a single junction. On each road the vehicle density evolves according to a scalar conservation law, and the requirements for joining the solutions at the junction are defined via the so-called vanishing viscosity germ. The algorithm mentioned above processes the junction in an implicit manner. We propose an explicit version of the algorithm. It differs only in the way that the junction is processed. We prove that the approximations converge to the unique entropy solution of the associated Cauchy problem.</p>


2017 ◽  
Vol 37 (11) ◽  
pp. 5913-5942 ◽  
Author(s):  
Boris P. Andreianov ◽  
◽  
Giuseppe Maria Coclite ◽  
Carlotta Donadello ◽  
◽  
...  

2018 ◽  
Vol 30 (1) ◽  
pp. 117-175 ◽  
Author(s):  
DOROTHEE KNEES ◽  
RICCARDA ROSSI ◽  
CHIARA ZANINI

This article is the third one in a series of papers by the authors on vanishing-viscosity solutions to rate-independent damage systems. While in the first two papers (Knees, D. et al. 2013 Math. Models Methods Appl. Sci.23(4), 565–616; Knees, D. et al. 2015 Nonlinear Anal. Real World Appl.24, 126–162) the assumptions on the spatial domain Ω were kept as general as possible (i.e., non-smooth domain with mixed boundary conditions), we assume here that ∂Ω is smooth and that the type of boundary conditions does not change. This smoother setting allows us to derive enhanced regularity spatial properties both for the displacement and damage fields. Thus, we are in a position to work with a stronger solution notion at the level of the viscous approximating system. The vanishing-viscosity analysis then leads us to obtain the existence of a stronger solution concept for the rate-independent limit system. Furthermore, in comparison to [18, 19], in our vanishing-viscosity analysis we do not switch to an artificial arc-length parameterization of the trajectories but we stay with the true physical time. The resulting concept of Balanced Viscosity solution to the rate-independent damage system thus encodes a more explicit characterization of the system behaviour at time discontinuities of the solution.


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