Tumor-immune cell interactions by a fully parabolic chemotaxis model with logistic source

Abstract

This work studies the existence of classical solutions to a class of chemotaxis systems reading \[\begin{cases} u_t = Δu-χ\nabla\cdot(u \nabla v) + μ_1 u^k -μ_2 u^{k+1}, & \text{in} \; Ω\times(0,T_{\text{max}}), \\ v_t= Δv+αw-βv-γu v, & \text{in} \; Ω\times(0,T_{\text{max}}), \\ w_t= Δw-δu w+ μ_3 w(1-w), & \text{in} \; Ω\times(0,T_{\text{max}}), \\ \frac{\partial u}{\partialν}=\frac{\partial v}{\partialν}=\frac{\partial w}{\partialν}=0, & \text{on} \; \partialΩ\times(0,T_{\text{max}}), \\ u(x,0)=u_0(x), \quad v(x,0)= v_0(x), \quad w(x,0)= w_0(x), & x\in\overlineΩ, \end{cases}\] that model interactions between tumor (i.e., $w$) and immune cells (i.e., $u$) with a logistic-type source term $μ_1 u^k - μ_2 u^{k+1}$, $k\geq1$, also in presence of a chemical signal (i.e., $v$). The model parameters $χ, μ_1,μ_2, μ_3, α, β, γ$, and $δ$ are all positive. The value $T_{\text{max}}$ indicates the maximum instant of time up to which solutions are defined. Our focus is on examining the global existence in a bounded domain $Ω\subset \mathbb{R}^n, n \geq 3$, under Neumann boundary conditions. We distinguish between two scenarios: $k>1$ and $k=1$. The first case allows to prove boundedness under smaller assumptions relying only on the model parameters instead of on the initial data, while the second case requires an extra condition relating the parameters $χ, μ_2$, $n$, and the initial data $\lVert v_0 \rVert_{L^\infty(Ω)}$. This model can be seen as an extension of those previously examined in [11] and [4], being the former a system with only two equations and the latter the same model without logistic.