The purpose of this note is to establish a new version of the local
Steiner formula
and to give an application to convex bodies of constant width. This variant
of the
Steiner formula generalizes results of Hann [3] and
Hug
[6], who use much less
elementary techniques than the methods of this paper. In fact, Hann asked
for a
simpler proof of these results [4, Problem 2, p. 900].
We remark that our formula
can be considered as a Euclidean analogue of a spherical result
proved in [2, p. 46],
and that our method can also be applied in hyperbolic space.
For some remarks on related formulas in certain two-dimensional Minkowski
spaces, see Hann [5, p. 363].
For further information about the notions used below,
we refer to Schneider's book [9]. Let
[Kscr ]n be the set of all convex bodies in Euclidean
space
IRn, that is, the
set of all compact, convex, non-empty subsets of IRn.
Let Sn-1 be the unit sphere. For
K∈[Kscr ]n, let NorK be the set
of all support
elements of K, that is, the pairs (x,
u)∈IRn×Sn−1
such that x is a boundary point of K and u is
an outer unit
normal vector of K at the point x. The support measures
(or
generalized curvature measures) of K, denoted by
Θ0(K, ·), …,
Θn−1(K, ·), are the unique
Borel measures
on IRn×Sn−1
that are
concentrated on NorK and satisfy
formula here
for all integrable functions f[ratio ]IRn→IR;
here λ denotes the Lebesgue measure on
IRn. Equation (1), which is a consequence and a
slight generalization of Theorem
4.2.1 in Schneider [9], is called the local Steiner
formula. Our main result is the following.