“…A formal asymptotic analysis is carried out in [22] to identify the corresponding sharp interface problem. The growth assumptions on the potential F and the proliferation function are more general than the ones in [8]. Our first main result is a well-posedness theorem for weak solutions which are just energy bounded.…”
Section: Discussionmentioning
confidence: 97%
“…The same contribution contains a numerical scheme as well as some numerical simulations. The first theoretical results concerning existence and uniqueness of solutions are proven in [8]. The first theoretical results concerning existence and uniqueness of solutions are proven in [8].…”
Section: Discussionmentioning
confidence: 99%
“…Numerical simulations of diffuse-interface model for tumour growth have been carried out in several papers (see, for instance, [11,Chap. Moreover, a very recent contribution (see [8]) is devoted to analyze an approximation of a model recently proposed in [21] (see also [22,35]). Nonetheless, a rigorous mathematical analysis of the resulting systems of differential equations is still in its infancy.…”
Section: Introductionmentioning
confidence: 99%
“…However, in this paper we suppose p to be, at least, Lipschitz continuous, but we allow it to satisfy a suitable growth condition (cf. (1.5) In [8], the authors consider a relaxed model in which the chemical potential μ contains a viscous term αϕ t , α > 0 and equation (1.1) has an additional term αμ t which requires a further initial condition. Also, it is worth observing that more general potentials F, possibly depending on ψ as well, might be taken into account since they are relevant from the modelling viewpoint (cf.…”
Section: Introductionmentioning
confidence: 99%
“…The assumptions on F and p are more general than the ones in [8] for the case α = 0. This is our first result, namely, existence of a weak solution of finite energy.…”
Link to this article: http://journals.cambridge.org/abstract_S0956792514000436How to cite this article: SERGIO FRIGERI, MAURIZIO GRASSELLI and ELISABETTA ROCCA (2015). On a diffuse interface model of tumour growth. We consider a diffuse interface model of tumour growth proposed by A. Hawkins-Daruud et al. ((2013) J. Math. Biol. 67 1457-1485). This model consists of the Cahn-Hilliard equation for the tumour cell fraction ϕ nonlinearly coupled with a reaction-diffusion equation for ψ, which represents the nutrient-rich extracellular water volume fraction. The coupling is expressed through a suitable proliferation function p(ϕ) multiplied by the differences of the chemical potentials for ϕ and ψ. The system is equipped with no-flux boundary conditions which give the conservation of the total mass, that is, the spatial average of ϕ + ψ. Here, we prove the existence of a weak solution to the associated Cauchy problem, provided that the potential F and p satisfy sufficiently general conditions. Then we show that the weak solution is unique and continuously depends on the initial data, provided that p satisfies slightly stronger growth restrictions. Also, we demonstrate the existence of a strong solution and that any weak solution regularizes in finite time. Finally, we prove the existence of the global attractor in a phase space characterized by an a priori bounded energy.
“…A formal asymptotic analysis is carried out in [22] to identify the corresponding sharp interface problem. The growth assumptions on the potential F and the proliferation function are more general than the ones in [8]. Our first main result is a well-posedness theorem for weak solutions which are just energy bounded.…”
Section: Discussionmentioning
confidence: 97%
“…The same contribution contains a numerical scheme as well as some numerical simulations. The first theoretical results concerning existence and uniqueness of solutions are proven in [8]. The first theoretical results concerning existence and uniqueness of solutions are proven in [8].…”
Section: Discussionmentioning
confidence: 99%
“…Numerical simulations of diffuse-interface model for tumour growth have been carried out in several papers (see, for instance, [11,Chap. Moreover, a very recent contribution (see [8]) is devoted to analyze an approximation of a model recently proposed in [21] (see also [22,35]). Nonetheless, a rigorous mathematical analysis of the resulting systems of differential equations is still in its infancy.…”
Section: Introductionmentioning
confidence: 99%
“…However, in this paper we suppose p to be, at least, Lipschitz continuous, but we allow it to satisfy a suitable growth condition (cf. (1.5) In [8], the authors consider a relaxed model in which the chemical potential μ contains a viscous term αϕ t , α > 0 and equation (1.1) has an additional term αμ t which requires a further initial condition. Also, it is worth observing that more general potentials F, possibly depending on ψ as well, might be taken into account since they are relevant from the modelling viewpoint (cf.…”
Section: Introductionmentioning
confidence: 99%
“…The assumptions on F and p are more general than the ones in [8] for the case α = 0. This is our first result, namely, existence of a weak solution of finite energy.…”
Link to this article: http://journals.cambridge.org/abstract_S0956792514000436How to cite this article: SERGIO FRIGERI, MAURIZIO GRASSELLI and ELISABETTA ROCCA (2015). On a diffuse interface model of tumour growth. We consider a diffuse interface model of tumour growth proposed by A. Hawkins-Daruud et al. ((2013) J. Math. Biol. 67 1457-1485). This model consists of the Cahn-Hilliard equation for the tumour cell fraction ϕ nonlinearly coupled with a reaction-diffusion equation for ψ, which represents the nutrient-rich extracellular water volume fraction. The coupling is expressed through a suitable proliferation function p(ϕ) multiplied by the differences of the chemical potentials for ϕ and ψ. The system is equipped with no-flux boundary conditions which give the conservation of the total mass, that is, the spatial average of ϕ + ψ. Here, we prove the existence of a weak solution to the associated Cauchy problem, provided that the potential F and p satisfy sufficiently general conditions. Then we show that the weak solution is unique and continuously depends on the initial data, provided that p satisfies slightly stronger growth restrictions. Also, we demonstrate the existence of a strong solution and that any weak solution regularizes in finite time. Finally, we prove the existence of the global attractor in a phase space characterized by an a priori bounded energy.
This article considers a limit system by passing to the limit in the following Cahn–Hilliard type phase‐field system related to tumor growth as β↘0:
α∂tμβ+∂tφβ−normalΔμβ=pfalse(σβ−μβfalse)in1emnormalΩ×false(0,Tfalse),μβ=β∂tφβ+false(−normalΔ+1false)φβ+ξβ+πfalse(φβfalse),1emξβ∈Bfalse(φβfalse)in1emnormalΩ×false(0,Tfalse),∂tσβ−normalΔσβ=−pfalse(σβ−μβfalse)in1emnormalΩ×false(0,Tfalse),
in a bounded or an unbounded domain
normalΩ⊂RN with smooth‐bounded boundary. Here,
N∈double-struckN, T > 0, α > 0, β > 0, p ≥ 0, B is a maximal monotone graph, and π is a Lipschitz continuous function. In the case that Ω is a bounded domain, p and −Δ + 1 are replaced with p(φβ) and −Δ, respectively, and p is a Lipschitz continuous function; Colli, Gilardi, Rocca, and Sprekels (Discrete Contin Dyn Syst Ser S 2017; 10:37–54) have proved existence of solutions to the limit problem with this approach by applying the Aubin–Lions lemma for the compact embedding H1(Ω)↪L2(Ω) and the continuous embedding L2(Ω)↪(H1(Ω))∗. However, the Aubin–Lions lemma cannot be applied directly when Ω is an unbounded domain. The present work establishes existence of weak solutions to the limit problem along with uniqueness and error estimates in terms of the parameter β↘0. To this end, we construct an applicable theory by noting that the embedding H1(Ω)↪L2(Ω) is not compact in the case that Ω is an unbounded domain.
We consider the sliding mode control (SMC) problem for a diffuse interface tumor growth model coupling a Cahn–Hilliard equation with a reaction–diffusion equation perturbed by a maximal monotone nonlinearity. We prove existence and regularity of strong solutions and, under further assumptions, a uniqueness result. Then, we show that the chosen SMC law forces the system to reach within finite time a sliding manifold that we chose in order that the tumor phase remains constant in time.
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