This article establishes a verification theorem for an optimal control problem governed by the two- and three-dimensional convective Brinkman--Forchheimer equations on the $d$-dimensional torus, $d\in\{2,3\}$: $$\frac{\partial\mathfrak{u}}{\partial t} -μΔ\mathfrak{u} +(\mathfrak{u}\cdot\nabla)\mathfrak{u} +α\mathfrak{u} +β|\mathfrak{u}|^{r-1}\mathfrak{u} +\nabla\mathfrak{p} =\boldsymbol{f}, \qquad \nabla\cdot\mathfrak{u}=0,$$ where $μ,α,β>0$ and $r\in[1,\infty)$. We derive the Pontryagin maximum principle and develop a verification framework for the associated control problem, a topic that has received comparatively little attention for fluid models of Navier--Stokes type. A major challenge in establishing the verification theorem and the corresponding feedback characterization for the CBF system is that the analysis requires a substantially different regularity framework from that used for the two-dimensional Navier--Stokes equations. In particular, the present approach relies on strong solution theory, a delicate treatment of the nonlinear absorption term, novel estimates in negative-order Sobolev spaces, and continuous dependence estimates in stronger topologies, especially in the three-dimensional setting. A distinctive feature of the present work is that the verification framework is developed not only in two dimensions, but also in the three-dimensional supercritical regime, corresponding to $r\in(3,5]$, and in the critical case $r=3$ under the condition $2βμ\geq1$. Consequently, the feedback characterization and verification arguments can be rigorously justified in both two and three dimensions.
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