We formulate in the language of linear algebra the intercept theorems. We work in the setting of a two-dimensional Euclidean vector space, which provides lengths of line segments. Two affine lines are called parallel if they are spanned by the same vector. We formulate the intercept theorems in such a way that the intersecting point of the rays lies in the origin. This can always be achieved by translating the intersecting point to the origin, as this does not change the lengths.
Let denote a two-dimensional
Euclidean vector space,
let
be vectors, and suppose that and are
linearly independent,
and that and are linearly independent. Let
and
denote the lines
(the rays)
defined by
and .
Let
and
be points in with the corresponding parallel lines
and
.
We denote the intersecting points
(which exist uniquely due to the condition)
by
Without loss of generality, we may assume that
,
,
and
,
as this does not change the lines involved. We write
.
We have
;
therefore, we obtain
This point belongs to and also to . This means that this point is just . Hence,
,
and
In particular, the preceding theorem says that in the given situation, the ratios of corresponding side lengths of the triangles
and
are the same. These triangles are similar; the triangle arises from the triangle by a homothety with factor . This factor describes all length relations.
An application of the intercept theorem. One can compute the width of the river without crossing the river.
Another application of the intercept theorem is to guess a distance using one thumb but two eyes.
Let denote a two-dimensional
Euclidean vector space,
let
be vectors, and suppose that and are
linearly independent,
and that and are linearly independent. Let
and
denote the lines defined by
and .
Let
and
be points in with the corresponding parallel lines
and
.
We denote the intersecting points
(which exist uniquely due to the condition)
by
Let be a two-dimensional
Euclidean vector space,
let
be vectors, and suppose that
is
linearly independent
to each of these vectors. Let
, ,
be the lines defined by the . Let
and
be points in with den corresponding parallel lines
and
. We denote the intersecting points of the lines
(which exist uniquely due to the conditions)
by