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Let us denote with the -dimensional Hausdorff measure in
.
A set
is said to be countably -rectifiable if there exists a countable sequence of Lipschitz continuous functions
such that
A set
is said to be countably -rectifiable if there exists a set which is countable -rectifiable and such that
.
A set
is said to be -rectifiable or simply -rectifiable if it is -rectifiable and
.
If is any Borel subset of
and
is given, one can define the density of in as
where is the Lebesgue measure of the unit ball in
. Notice that an -dimensional plane has density in all points and density 0 in all points
.
It turns out that if is rectifiable, then in -a.e. point the density
exists and is equal to . Moreover in -a.e. point there exists an approximate tangent plane to as defined below.
Given a point
and a vector
we say that is tangent to in if there exists a sequence of points , and a sequence of positive numbers such that
If is an -dimensional manifold, then the set of tangent vectors to a point is nothing else than the usual tangent plane to in .
We say that a vector is approximately tangent to in if it is a tangent vector to every subset of such that
. Notice that every tangent vector is also an approximately tangent vector while the converse is not always true, as it is shown in an example below. The point, here, is that being the set defined -almost everywhere, we need a stronger definition for tangent vectors.
The approximate tangent cone to in is the set of all approximately tangent vectors to in (notice that if is a tangent vector then is also a tangent vector, for all ). If the approximate tangent cone is an -dimensional vector subspace of
, it is called the approximate tangent plane.
Notice that if
is any -dimensional regular surface, and is the set of all points of
with rational coordinates, then the set is an -rectifiable set since
. Notice, however, that
and consequently every vector is tangent to in every point
. On the other hand the approximately tangent vectors to are only the tangent vectors to , because the set has density 0 everywhere.
- 1
- Frank Morgan: Geometric Measure Theory: A Beginner's Guide.
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