mixed volume
In mathematics, more specifically, in convex geometry, the mixed volume is a way to associate a non-negative number to a tuple of convex bodies in . This number depends on the size and shape of the bodies, and their relative orientation to each other.
Definition
Let be convex bodies in and consider the function
:
= \mathrm{Vol}_n (\lambda_1 K_1 + \cdots + \lambda_r K_r), \qquad \lambda_i \geq 0,
where stands for the -dimensional volume, and its argument is the Minkowski sum of the scaled convex bodies . One can show that is a homogeneous polynomial of degree , so can be written as
:
= \sum_{j_1, \ldots, j_n = 1}^r V(K_{j_1}, \ldots, K_{j_n})
\lambda_{j_1} \cdots \lambda_{j_n},
where the functions are symmetric. For a particular index function , the coefficient is called the mixed volume of .
Properties
- The mixed volume is uniquely determined by the following three properties:
V(K, \dots, K) =\text{Vol}_n (K);
- is symmetric in its arguments;
- is multilinear:
V(\lambda K + \lambda' K', K_2, \dots, K_n) = \lambda V(K, K_2, \dots, K_n)
+ \lambda' V(K', K_2, \dots, K_n) for
\lambda,\lambda' \geq 0.
- The mixed volume is non-negative and monotonically increasing in each variable:
V(K_1, K_2, \ldots, K_n) \leq V(K_1', K_2, \ldots, K_n) for
K_1 \subseteq K_1'.
- The Alexandrov–Fenchel inequality, discovered by Aleksandr Danilovich Aleksandrov and Werner Fenchel:
::
:Numerous geometric inequalities, such as the Brunn–Minkowski inequality for convex bodies and Minkowski's first inequality, are special cases of the Alexandrov–Fenchel inequality.
Quermassintegrals
Let be a convex body and let be the Euclidean ball of unit radius. The mixed volume
:
is called the j-th quermassintegral of .{{cite journal|mr=1089383|last=McMullen|first=Peter|authorlink=Peter McMullen|title=Inequalities between intrinsic volumes|journal=Monatshefte für Mathematik|volume=111|year=1991|issue=1|pages=47–53|doi=10.1007/bf01299276|doi-access=free}}
The definition of mixed volume yields the Steiner formula (named after Jakob Steiner):
:
= \sum_{j=0}^n \binom{n}{j} W_j(K) t^j.
=Intrinsic volumes=
The j-th intrinsic volume of is a different normalization of the quermassintegral, defined by
: or in other words
where is the volume of the -dimensional unit ball.
=Hadwiger's characterization theorem=
{{main|Hadwiger's theorem}}
Hadwiger's theorem asserts that every valuation on convex bodies in that is continuous and invariant under rigid motions of is a linear combination of the quermassintegrals (or, equivalently, of the intrinsic volumes).{{cite journal|mr=1376731|last=Klain|first=Daniel A.|title=A short proof of Hadwiger's characterization theorem|journal=Mathematika|volume=42|year=1995|issue=2|pages=329–339|doi=10.1112/s0025579300014625}}
Notes
{{Reflist}}
External links
{{eom|id=Mixed-volume_theory|title=Mixed-volume theory|first=Yu.D.|last=Burago}}