“…To sketch the relation between the polygonal Riesz inequality and the physical isoperimetric inequalities (4), let us focus for simplicity on the Saint-Venant inequality. It is known that the torsional rigidity satisfies (see [17,Section 4]) (6) τ (Ω) = A probabilistic reformulation in the same vein can be given also for the principal frequency, see again [17,Section 4]. Then the classical Saint-Venant and Faber-Krahn inequalities, with the ball as optimal domain, can be obtained as a consequence of the general rearrangement inequality for multiple integrals due to Brascamp-Lieb-Luttinger [8, Theorem 1.2], which in 2-dimensions reads here h i are measurable non-negative functions on R 2 vanishing at infinity, h * i are their symmetric decreasing rearrangements, {a ij } are real numbers, Ω is a set of finite Lebesgue measure in R 2 , and Ω * is the ball with the same area as Ω.…”