Abstract

For this paper, we are interested in network formation of endothelial cells. Randomly distributed endothelial cells converge together to create a vascular system. To develop a mathematical model, we make assumptions on individual cell movement, leading to a velocity jump model with chemotaxis. We use scaling arguments to derive an anisotropic chemotaxis model on the population level. For this macroscopic model, we develop a new numerical solver and investigate network-type pattern formation. Our model is able to reproduce experiments on network formation by Serini et al. Moreover, to our surprise, we found new spatial criss-cross patterns due to competing cues, one direction given by tissue anisotropy versus a different direction due to chemotaxis. A full analysis of these new patterns is left for future work.

Highlights

  • Network formation is an important process in many biological tissues

  • The spatial interaction of moving endothelial cells leads to a spontaneous network formation, in a process that is not based on a trail following mechanism but rather arises as macroscopic pattern formation in a chemotaxis system

  • We analyzed two effects that can lead to directional orientation of moving particles: chemotaxis and anisotropy

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Summary

Introduction

Network formation is an important process in many biological tissues. For example, in angiogenesis, blood vessels sprout and grow to form functioning vascular networks [1], or lung tissue, which forms a complex network of bronchioli. The spatial interaction of moving endothelial cells leads to a spontaneous network formation, in a process that is not based on a trail following mechanism but rather arises as macroscopic pattern formation in a chemotaxis system. In this paper, we generalize Serini’s et al approach and consider a chemotaxis-transport equation model, which is based on detailed microscopic cell movement patterns often referred to as “run and tumble” [9,10,11,12,13]. The anisotropic chemotaxis model balances two causes of anisotropy, the directionality of the underlying tissue and the orientation of the chemotactic gradient These two effects compete, leading to interesting criss-cross patterns, which have never been observed before in a mathematical model.

Background
Transport Equations
Chemotaxis-Transport Equations
Parabolic Scaling
Numerics
Hybrid FVFD Scheme
Parameters
Scheme Test
Vascular Network Formation
Anisotropic Diffusion
Chemotactic Mixing
Entrapment by Fibres
Findings
Discussion

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