The Neumann initial-boundary problem for the chemotaxis system \begin{align} \label{prob:abstract} \tag{} \begin{cases} u_t = \Delta u - \nabla \cdot (u \nabla v) + \kappa(|x|) u - \mu(|x|) u^p, \ 0 = \Delta v - \frac{m(t)}{|\Omega|} + u, \quad m(t) := \int_\Omega u(\cdot, t) \end{cases} \end{align} is studied in a ball $\Omega = B_R(0) \subset \mathbb R^2R \gt 0p \ge 1\kappa, \mu: [0, R] \rightarrow [0, \infty)$. We prove that whenever as well as $\mu(s) \le \mu_1 s^{2p-2}s \in [0, R]\mu_1 \gt 0m_0 \gt 8 \piu_0 \in C^0(\overline \Omega)\int_\Omega u_0 = m_0(u, v)u_0\kappa \equiv 0$ then all solutions with initial mass smaller than are global in time, displaying a certain critical mass phenomenon. On the other hand, if , we show that for all satisfying for all and some $\mu_1, \varepsilon \gt 0$ the system \eqref{prob:abstract} admits a global classical solution for each initial datum

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