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Hyperbolic triangle

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A hyperbolic triangle is a fundamental shape within the hyperbolic plane. It is defined by three non-collinear points, known as vertices, and the three segments connecting them, known as sides or edges.

Hyperbolic triangle
Hyperbolic triangle

While these triangles exist in a curved space, any three points in a hyperbolic space of any dimension will always lie on the same plane. This allows mathematicians to study planar hyperbolic triangles even when working in much higher dimensions. These shapes are essential for understanding non-Euclidean geometry, where the rules of flat space no longer apply.

To understand how these triangles function, one must look at their unique geometric properties. Every hyperbolic triangle possesses an inscribed circle, which is a circle that fits perfectly inside the triangle. However, not every hyperbolic triangle has a circumscribed circle that passes through all three vertices. This occurs if at least one vertex is an ideal point, or if the vertices lie on a horocycle or a one-sided hypercycle. Furthermore, hyperbolic triangles are characterized as being "thin." This means there is a maximum distance, denoted as delta, from any point on an edge to one of the other two edges. This specific characteristic led to the mathematical concept of delta-hyperbolic space.

Hyperbolic triangles exhibit several distinct types based on their vertices. A special category includes triangles with ideal vertices, where the corners sit on the ideal boundary of the plane. If two sides are limiting parallel, they approach each other but never intersect, forming an angle of zero at an omega point. A triangle with exactly one ideal vertex is called an omega triangle. Another specific type is the triangle of parallelism, which has one ideal vertex and one right angle. Ferdinand Karl Schweikart described the Schweikart triangle in 1818, which features two ideal vertices and one right angle. Finally, an ideal triangle has all three vertices at the ideal boundary. Because its angles all sum to zero, it is the largest possible triangle in hyperbolic geometry.

The history of these shapes is tied to the discovery of how curvature affects geometry. Johann Heinrich Lambert first proved a vital theorem relating a triangle's area to its angle sum. In Euclidean geometry, the angles of a triangle always sum to 180 degrees. In hyperbolic geometry, the sum of the angles A, B, and C is always strictly less than 180 degrees. This difference is known as the defect of the triangle. The area of a hyperbolic triangle is directly proportional to this defect. Specifically, the area equals the defect multiplied by the square of the Gaussian curvature constant. This relationship is mathematically similar to Girard's theorem used in spherical geometry.

Mathematicians use various planar models to visualize these complex shapes on a flat surface. One common method is the Poincaré disk model, where the hyperbolic plane is contained within a unit circle. In this model, hyperbolic lines appear as the interior parts of circles that intersect the unit circle at right angles.

Ideal circles
Ideal circles

Another method is the Poincaré half-plane model, which uses the upper half of the complex plane. In this model, the real axis acts as the boundary at infinity, and hyperbolic lines are represented by circles or lines that intersect the real axis at right angles. These models allow for the use of Möbius transformations to move shapes without changing their fundamental properties.

Trigonometry in the hyperbolic plane relies on different functions than those used in flat geometry. Instead of standard sine and cosine, hyperbolic trigonometry uses hyperbolic functions such as sinh, cosh, and tanh. These formulas depend on measuring sides in absolute length, which is a unit that sets the Gaussian curvature to negative one. For a right triangle with angle C as the right angle, the sine of angle A is the hyperbolic sine of the opposite side divided by the hyperbolic sine of the hypotenuse. There are also complex laws, such as the hyperbolic law of cosines and the hyperbolic law of sines, which allow for the calculation of sides and angles in any hyperbolic triangle.

The study of hyperbolic triangles reveals deep connections to other mathematical fields. There is a striking analogy between hyperbolic and spherical trigonometry. If one replaces the sides in spherical formulas with imaginary values, the formulas transform into hyperbolic ones. This connection shows that these geometries are part of a larger, interconnected system. Hyperbolic geometry also allows for the creation of complex, repeating patterns known as tilings.

Order-7 triangular tiling
Order-7 triangular tiling

These tilings, such as an order-7 triangular tiling, demonstrate how equilateral triangles can fill a hyperbolic plane in ways that are impossible in flat space.

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File:Hyperbolic triangle.svg
Hyperbolic triangle.svg
File:Order-7 triangular tiling.svg
Order-7 triangular tiling.svg
File:Ideal circles.svg
Ideal circles.svg
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