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Gruber P. Convex and Discrete Geometry

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Fig. 9.3. Rearrangement of functions<br />

9 Symmetrization 179<br />

The following rearrangement theorem is indispensable for certain isoperimetric<br />

inequalities of mathematical physics, see the next section. While this result was<br />

known <strong>and</strong> used at least since Faber [316] <strong>and</strong> Krahn [615], a complete proof requires<br />

tools of more recent geometric measure theory. See Talenti [987] for its history <strong>and</strong><br />

references to proofs. Compare also B<strong>and</strong>le [64]. Here no proof is presented.<br />

Theorem 9.7. Let f : Ed →[0, +∞) be locally Lipschitz <strong>and</strong> such that f (x) → 0<br />

as �x� →∞. Then f r : Ed →[0, +∞) is also locally Lipschitz, f r (x) → 0 as<br />

�x� →∞, <strong>and</strong><br />

�<br />

�<br />

� �2dx � � r 2dx.<br />

grad f (x) ≥ grad f (x)<br />

E d<br />

(Since f <strong>and</strong> f r are locally Lipschitz, (grad f ) 2 <strong>and</strong> (grad f r ) 2 are measurable <strong>and</strong><br />

exist almost everywhere, see [696].)<br />

9.4 Torsional Rigidity <strong>and</strong> Minimum Principal Frequency<br />

We begin with the following quotation from B<strong>and</strong>le [64], preface.<br />

The study of ‘isoperimetric inequalities’ in a broader sense began with the conjecture<br />

of St Venant in 1856. Investigating the torsion of elastic prisms, he observed<br />

that of all cross-sections of given area the circle has the maximal torsional rigidity.<br />

This conjecture was proved by Pólya in 1948. Lord Rayleigh conjectured that of<br />

all membranes with given area, the circle has the smallest principal frequency. This<br />

statement was proved independently by Faber <strong>and</strong> Krahn around 1923.<br />

There is a large body of isoperimetric type inequalities in mathematical physics<br />

dealing with eigenvalues of partial differential equations. In physical terms these<br />

inequalities concern principal frequencies of membranes, torsional rigidity, bending<br />

of beams, electrostatic capacity, etc. Major contributors are Saint-Venant, Faber,<br />

Krahn, Pólya <strong>and</strong> Szegö, Osserman, Hersch, Payne, Talenti <strong>and</strong> others.<br />

The above rearrangement theorem will be applied to give the best upper, respectively,<br />

lower, bound for the torsional rigidity of an elastic cylindrical rod <strong>and</strong> for the<br />

first principal frequency of a clamped membrane.<br />

For more information, see the surveys <strong>and</strong> books of Pólya <strong>and</strong> Szegö [811],<br />

B<strong>and</strong>le [64], Mossino [757], Hersch [498], Payne [786] <strong>and</strong> Talenti [987].<br />

E d

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