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Affine geometry

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Affine geometry is a branch of mathematics that studies the properties of shapes that remain unchanged even when those shapes are stretched, tilted, or slid across a plane. In standard Euclidean geometry, mathematicians focus on exact measurements like the length of a side or the degree of an angle. Affine geometry, however, chooses to "forget" these metric notions. Instead, it focuses on the relationships between points and lines. Specifically, it is often described as the study of parallel lines. This is because the concept of parallelism does not depend on measuring distances or angles, making it a fundamental part of the affine system.

To understand how this works, we must look at the mechanics of affine transformations. An affine transformation is a mapping that preserves two specific things: the alignment of points and the parallelism of lines. This means if three points sit on a single straight line, they will still sit on a single straight line after the transformation. Similarly, if two lines are parallel before the move, they will remain parallel afterward. These transformations include translations, which are simply shifts from one position to another. They also include more complex movements that can change the proportions of a shape without breaking its basic structure.

Translation parallelogram
Translation parallelogram

There are two primary ways to develop the rules of affine geometry. The first is through synthetic geometry. In this approach, an affine space is defined as a set of points and lines that follow specific axioms. One of the most important rules is Playfair's axiom. This axiom states that if you have a line and a point not on that line, there is exactly one line through that point that is parallel to the first line. Another important rule is Pappus' law. This law describes a specific relationship between sets of parallel lines. If certain lines are parallel in a specific pattern, then other lines in that pattern must also be parallel.

PappusAffine.2
PappusAffine.2

The second method is through linear algebra. In this context, an affine space is viewed as a set of points connected to a vector space. A vector is a mathematical object that represents a direction and a magnitude, which can be used to perform translations. In an affine space, you can use a vector to move one point to another. While you can pick any point to act as an "origin" or a starting point, there is no single preferred choice. You can think of an affine space as a vector space where the specific location of the zero vector, or origin, has been forgotten.

Translation parallelogram
Translation parallelogram

The history of these ideas spans several centuries of mathematical discovery. The term "affine" was first introduced by Leonhard Euler in 1748 in his book *Elements of Analytical Geometry*. Later, in 1827, August Möbius explored these concepts in his own writings. In the early 20th century, Felix Klein's Erlangen program helped mathematicians recognize affine geometry as a generalization of Euclidean geometry. In 1918, Hermann Weyl used affine geometry in his text *Space, Time, Matter*. Weyl used these principles to introduce the concepts of vector addition and subtraction, which were vital for his work in mathematical physics.

PappusAffine.2
PappusAffine.2

Affine geometry provides powerful tools for solving geometric problems through affine invariants. An invariant is something that stays the same even after a transformation. For example, the ratio of areas in certain shapes is an affine invariant. If you have a triangle, the lines that divide its area into two equal halves will always form a specific shape inside the triangle. The ratio of the area of this internal shape to the area of the triangle is always approximately 0.019860. This remains true no matter how much you stretch or tilt the triangle. Other important invariants include formulas for area and volume, such as the rule that a triangle's area is half the base times the height.

Translation parallelogram
Translation parallelogram

Beyond pure math, these concepts connect deeply to the study of motion, known as kinematics. In classical Newtonian physics, scientists use affine transformations called shear mappings to describe how an observer sees movement. However, when studying the universe at high speeds, researchers must account for the finite speed of light. In 1912, Edwin B. Wilson and Gilbert N. Lewis used affine geometry to help develop a modern understanding of space-time. Their work showed how different types of mappings can describe the complex relationship between time and space in the special theory of relativity.

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File:Translation parallelogram.svg
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File:PappusAffine.2.svg
PappusAffine.2.svg
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