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Mixed volume

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In mathematics, more specifically, in convex geometry, the mixed volume is a way to associate a non-negative number to an n-tuple of convex bodies in the n-dimensional space. This number depends on the size of the bodies as well as their relative position.[1]

Definition

Let K1K2, ..., Kr be convex bodies in Rn, and consider the function

of non-negative λ-s, where Voln stands for the n-dimensional volume. One can show that f is a homogeneous polynomial of degree n, therefore it can be written as

where the functions V are symmetric. Then V(T1, ..., Tn) is called the mixed volume of T1T2, ..., Tn.

Equivalently,

Properties

  • The mixed volume is uniquely determined by the following three properties:
  1. V(T, ...., T) = Voln(T);
  2. V is symmetric in its arguments;
  3. V is multilinear: V(a T+b ST2, ..., Tn) =a V(TT2, ..., Tn)+b V(ST2, ..., Tn) for a,b ≥ 0.
  • The mixed volume is non-negative, and increasing in each variable.

Quermassintegrals

Let KRn be a convex body, and let BRn be the Euclidean ball. The mixed volume

is called the j-th quermassintegral of K.[2]

The definition of mixed volume yields the Steiner formula (named after Jakob Steiner):

Intrinsic volumes

The j-th intrinsic volume of K is defined by

where κn-j is the volume of the (n-j)-dimensional ball.

Hadwiger's characterization theorem

Hadwiger's theorem asserts that every valuation (measure theory) on convex bodies in Rn that is continuous and invariant under rigid motions of Rn is a linear combination of the quermassintegrals (or, equivalently, of the intrinsic volumes).[3]

Notes

  1. ^ Burago, Yu.D. (2001) [1994], "Mixed volume theory", Encyclopedia of Mathematics, EMS Press
  2. ^ McMullen, P. (1991). "Inequalities between intrinsic volumes". Monatsh. Math. 111 (1): 47–53. MR 1089383.
  3. ^ Klain, D.A. (1995). "A short proof of Hadwiger's characterization theorem". Mathematika. 42 (2): 329–339. MR 1376731.