For bounded, convex sets Omega subset mathbb {R}^d, the sharp Poincaré constant C(Omega ), which appears in ||f-bar{f}_{_{Omega }}||_{L^{infty }(Omega )} le C(Omega )||nabla f||_{L^{infty }(Omega )}, is given by C(Omega )=max _{_{partial Omega }}zeta for a specific convex function zeta [Bevan et al. in Proc Am Math Soc 151:1071–1085, 2023 (Theorem 1.1)]. We study C(cdot ) as a function on convex sets, in particular on polyhedra, and find that while a geometric characterization of C(Omega ) for triangles is possible, for other polyhedra the problem of ordering zeta (V_i), where V_i are the vertices of Omega , can be formidable. In these cases, we develop estimates of C(Omega ) from above and below in terms of more tractable quantities. We find, for example, that a good proxy for C(Q) when Q is a planar polygon with vertices V_i and centroid gamma (Q) is the quantity D(Q)=max _{i}|V_i-gamma (Q)|, with an error of up to sim 8%. A numerical study suggests that a similar statement holds for k-gons, this time with a maximal error across all k-gons of sim 13%. We explore the question of whether there is, for each Omega , at least one point M capable of ordering the zeta (V_i) according to the ordering of the |V_i-M|. For triangles, M always exists; for quadrilaterals, M seems always to exist; for 5-gons and beyond, they seem not to.