A phase field model for tumour growth is introduced that is based on a Brinkman law for convective velocity fields. The model couples a convective Cahn–Hilliard equation for the evolution of the tumour to a reaction-diffusion-advection equation for a nutrient and to a Brinkman–Stokes type law for the fluid velocity. The model is derived from basic thermodynamical principles, sharp interface limits are derived by matched asymptotics and an existence theory is presented for the case of a mobility which degenerates in one phase leading to a degenerate parabolic equation of fourth order. Finally numerical results describe qualitative features of the solutions and illustrate instabilities in certain situations.
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Typical situation for the formal asymptotic analysis
The tumour and healthy regions
Schematic sketch of the inner region close to
Initial tumour size for initial data
Comparison of Cahn--Hilliard--Darcy and Cahn--Hilliard--Brinkman models: Tumour at time
Influence of different mobilities: Tumour at time
Influence of the adhesion parameter
Influence of viscosiy I: Tumour and velocity for
Influence of viscosity II: Evolution of the tumour at time
Velocity profiles for different viscosities: The velocity magnitude at time
Influence of viscosity contrast: Tumour at time
Influence of initial profile I: Tumour at time
Influence of initial profile II: Tumour at time
Influence of initial profile III: Tumour at time
Influence of initial profile IV: Tumour at time