In geometry, the mean width is a measure of the "size" of a body; see Hadwiger's theorem for more about the available measures of bodies. In
n
(n-1)
\hat{n}
Sn-1
Sn
(n+1)
\hat{n}
\hat{n}
Sn-1
More formally, define a compact body B as being equivalent to set of points in its interior plus the points on the boundary (here, points denote elements of
Rn
hB(n)=max\{\langlen,x\rangle|x\inB\}
where
n
\langle,\rangle
Rn
b(B)= | 1 |
Sn-1 |
\int | |
Sn-1 |
hB(\hat{n})+hB(-\hat{n}),
where
Sn-1
(n-1)
Sn-1
The mean width of a line segment L is the length (1-volume) of L.
The mean width w of any compact shape S in two dimensions is p/π, where p is the perimeter of the convex hull of S. So w is the diameter of a circle with the same perimeter as the convex hull.
For convex bodies K in three dimensions, the mean width of K is related to the average of the mean curvature, H, over the whole surface of K. In fact,
\int\delta
H | |
2\pi |
dS=b(K)
where
\deltaK
K
dS
H
\deltaK
The mean width is usually mentioned in any good reference on convex geometry, for instance, Selected topics in convex geometry by Maria Moszyńska (Birkhäuser, Boston 2006). The relation between the mean width and the mean curvature is also derived in that reference.
The application of the mean width as one of the measures featuring in Hadwiger's theoremis discussed in Beifang Chen in "A simplified elementary proof of Hadwiger's volume theorem." Geom. Dedicata 105 (2004), 107—120.