- Saint-Venant's theorem
In
solid mechanics , it is common to analyze the properties of beams with constant cross section. Saint-Venant's theorem states that thesimply connected cross section with maximal torsionalrigidity is a circle. E. Makai, A proof of Saint-Venant's theorem on torsional rigidity, Acta Mathematica Hungarica, Volume 17, Numbers 3-4 / September, 419-422,1966DOI|10.1007/BF01894885 ] It is named after the French mathematicianAdhémar Jean Claude Barré de Saint-Venant .Given a
simply connected domain "D" in the plane with area "A" , ho the radius and sigma the area of its greatest inscribed circle, the torsional rigidity "P" of "D" is defined by:P= mathrm{sup}_f frac{left( intintlimits_D f, dx, dy ight)^2}{intintlimits_D f_x^2+f_y^2, dx, dy}Saint-Venant Saint-Venant [A J-C Barre de Saint-Venant, Memoire sur la torsion des prismes, Memoires presentes par divers savants a l'Acaddmie des Sciences, 14 (1856), pp. 233--560.] conjectured in 1856 thatof all domains "D" of equal area "A" the circular one has the greatest torsional rigidity, that is:P le P_{mathrm{circle le frac{A^2}{2 pi} a rigorous proof of this inequality was not given until 1948 by
Polya [G. Polya, Torsional rigidity, principal frequency, electrostatic capacity and symmetrization, Quarterly of Applied Math., 6 (1948), pp. 267 277.] . Another proof was given by Davenport and reported in [G. Polya and G. Szego, Isoperimetric inequalities in Mathematical Physics (Princeton Univ.Press, 1951).] . A more general proof and an estimate :P< 4 ho^2 AReferences
Wikimedia Foundation. 2010.