In solid mechanics, it is common to analyze the properties of beams with constant cross section.
Saint-Venant's theorem states that the simply connected cross section with maximal torsional rigidity is a circle.
[1] It is named after the French mathematician Adhémar Jean Claude Barré de Saint-Venant.
the area of its greatest inscribed circle, the torsional rigidity P of D is defined by Here the supremum is taken over all the continuously differentiable functions vanishing on the boundary of D. The existence of this supremum is a consequence of Poincaré inequality.
Saint-Venant[2] conjectured in 1856 that of all domains D of equal area A the circular one has the greatest torsional rigidity, that is A rigorous proof of this inequality was not given until 1948 by Pólya.