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 ${\displaystyle \mathbb {R} ^{n))$. This number depends on the size and shape of the bodies, and their relative orientation to each other.

Definition

Let ${\displaystyle K_{1},K_{2},\dots ,K_{r))$ be convex bodies in ${\displaystyle \mathbb {R} ^{n))$ and consider the function

${\displaystyle f(\lambda _{1},\ldots ,\lambda _{r})=\mathrm {Vol} _{n}(\lambda _{1}K_{1}+\cdots +\lambda _{r}K_{r}),\qquad \lambda _{i}\geq 0,}$

where ${\displaystyle {\text{Vol))_{n))$ stands for the ${\displaystyle n}$-dimensional volume, and its argument is the Minkowski sum of the scaled convex bodies ${\displaystyle K_{i))$. One can show that ${\displaystyle f}$ is a homogeneous polynomial of degree ${\displaystyle n}$, so can be written as

${\displaystyle f(\lambda _{1},\ldots ,\lambda _{r})=\sum _{j_{1},\ldots ,j_{n}=1}^{r}V(K_{j_{1)),\ldots ,K_{j_{n)))\lambda _{j_{1))\cdots \lambda _{j_{n)),}$

where the functions ${\displaystyle V}$ are symmetric. For a particular index function ${\displaystyle j\in \{1,\ldots ,r\}^{n))$, the coefficient ${\displaystyle V(K_{j_{1)),\dots ,K_{j_{n)))}$ is called the mixed volume of ${\displaystyle K_{j_{1)),\dots ,K_{j_{n))}$.

Properties

• The mixed volume is uniquely determined by the following three properties:

1. ${\displaystyle V(K,\dots ,K)={\text{Vol))_{n}(K)}$;
2. ${\displaystyle V}$ is symmetric in its arguments;
3. ${\displaystyle V}$ is multilinear: ${\displaystyle V(\lambda K+\lambda 'K',K_{2},\dots ,K_{n})=\lambda V(K,K_{2},\dots ,K_{n})+\lambda 'V(K',K_{2},\dots ,K_{n})}$ for ${\displaystyle \lambda ,\lambda '\geq 0}$.

• The mixed volume is non-negative and monotonically increasing in each variable: ${\displaystyle V(K_{1},K_{2},\ldots ,K_{n})\leq V(K_{1}',K_{2},\ldots ,K_{n})}$ for ${\displaystyle K_{1}\subseteq K_{1}'}$.
• The Alexandrov–Fenchel inequality, discovered by Aleksandr Danilovich Aleksandrov and Werner Fenchel:

${\displaystyle V(K_{1},K_{2},K_{3},\ldots ,K_{n})\geq {\sqrt {V(K_{1},K_{1},K_{3},\ldots ,K_{n})V(K_{2},K_{2},K_{3},\ldots ,K_{n}))).}$

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 ${\displaystyle K\subset \mathbb {R} ^{n))$ be a convex body and let ${\displaystyle B=B_{n}\subset \mathbb {R} ^{n))$ be the Euclidean ball of unit radius. The mixed volume

${\displaystyle W_{j}(K)=V({\overset {n-j{\text{ times))}{\overbrace {K,K,\ldots ,K} )),{\overset {j{\text{ times))}{\overbrace {B,B,\ldots ,B} )))}$

is called the j-th quermassintegral of ${\displaystyle K}$.^[1]

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

${\displaystyle \mathrm {Vol} _{n}(K+tB)=\sum _{j=0}^{n}{\binom {n}{j))W_{j}(K)t^{j}.}$

Intrinsic volumes

The j-th intrinsic volume of ${\displaystyle K}$ is a different normalization of the quermassintegral, defined by

${\displaystyle V_{j}(K)={\binom {n}{j)){\frac {W_{n-j}(K)}{\kappa _{n-j))},}$ or in other words ${\displaystyle \mathrm {Vol} _{n}(K+tB)=\sum _{j=0}^{n}V_{j}(K)\,\mathrm {Vol} _{n-j}(tB_{n-j}).}$

where ${\displaystyle \kappa _{n-j}={\text{Vol))_{n-j}(B_{n-j})}$ is the volume of the ${\displaystyle (n-j)}$-dimensional unit ball.

Hadwiger's characterization theorem

Hadwiger's theorem asserts that every valuation on convex bodies in ${\displaystyle \mathbb {R} ^{n))$ that is continuous and invariant under rigid motions of ${\displaystyle \mathbb {R} ^{n))$ is a linear combination of the quermassintegrals (or, equivalently, of the intrinsic volumes).^[2]