The reaction–cross‐diffusion models for tissue growth

Author(s):  
Zehra Pinar
2020 ◽  
Vol 22 (2) ◽  
pp. 175-203
Author(s):  
Martin Burger ◽  
José Carrillo ◽  
Jan-Frederik Pietschmann ◽  
Markus Schmidtchen

2018 ◽  
Vol 28 (11) ◽  
pp. 2097-2102 ◽  
Author(s):  
N. Bellomo ◽  
Y. Tao ◽  
M. Winkler

A presentation of a special issue on the derivation of cross-diffusion models and on the related analytical problems is proposed in this note. A brief introduction to motivations and recently published literature is presented in the first part. Subsequently, a concise description of the contents of the papers published in the issue follows. Finally, some ideas on possible research perspectives are proposed.


2020 ◽  
Vol 30 (06) ◽  
pp. 1033-1039
Author(s):  
N. Bellomo ◽  
Y. Tao ◽  
M. Winkler

A presentation of a special issue is delivered by this editorial paper on the derivation and related analytical problems, of cross diffusion models in complex environments. A brief introduction to motivations toward this research topic is presented in the first part. Subsequently, a concise description of the contents follows. Lastly, some ideas on possible research perspectives are proposed mainly focusing on modeling topics.


2018 ◽  
Vol 50 (5) ◽  
pp. 5695-5718 ◽  
Author(s):  
J. A. Carrillo ◽  
S. Fagioli ◽  
F. Santambrogio ◽  
M. Schmidtchen

2019 ◽  
Vol 29 (02) ◽  
pp. 237-270 ◽  
Author(s):  
Xiuqing Chen ◽  
Ansgar Jüngel

The weak–strong uniqueness for renormalized solutions to reaction–cross-diffusion systems in a bounded domain with no-flux boundary conditions is proved. The system generalizes the Shigesada–Kawasaki–Teramoto population model to an arbitrary number of species. The diffusion matrix is neither symmetric nor positive definite, but the system possesses a formal gradient-flow or entropy structure. No growth conditions on the source terms are imposed. It is shown that any renormalized solution coincides with a strong solution with the same initial data, as long as the strong solution exists. The proof is based on the evolution of the relative entropy modified by suitable cutoff functions.


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