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Intercept theorems/Linear algebra/Section

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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

and suppose that . Then

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

and suppose that . Then

This follows directly from fact.


In particular, we have the equation

which only takes the lengths on the rays into account.


In the last variant of the intercept theorem, there are three rays.


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

and suppose that . Then

We apply fact twice, to the situation given by and to the situation given by , and we obtain