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The Lambert Quadrilateral

Exploring the profound implications of three right angles in non-Euclidean geometries.

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Introduction

Definition

In the realm of geometry, a Lambert quadrilateral, also recognized as an Ibn al-Haytham–Lambert quadrilateral, is a specific type of quadrilateral possessing precisely three right angles.[1][2] This geometric figure holds significant historical importance, particularly concerning the Euclidean parallel postulate.

Historical Significance

Historically, the nature of the fourth angle in a Lambert quadrilateral was a subject of intense study. Mathematicians hypothesized that if the fourth angle could be proven to be a right angle, it would serve as a proof for the Euclidean parallel postulate. However, it is now understood that the measure of the fourth angle is contingent upon the specific geometric space in which the quadrilateral resides.

Relation to Saccheri Quadrilaterals

A Lambert quadrilateral can be elegantly constructed from a Saccheri quadrilateral. By connecting the midpoints of the base and the summit of a Saccheri quadrilateral, the resulting line segment is perpendicular to both. Each half of the Saccheri quadrilateral, thus formed, constitutes a Lambert quadrilateral.

Historical Context

The Quest for the Parallel Postulate

The study of quadrilaterals with three right angles dates back centuries, intrinsically linked to the efforts to prove Euclid's fifth postulate (the parallel postulate). Early mathematicians, including figures like Ibn al-Haytham (Alhazen), explored these shapes. The challenge was to demonstrate that in Euclidean geometry, a quadrilateral with three right angles must necessarily have a fourth right angle. This would have validated the parallel postulate without relying on its axiomatic assumption.

Non-Euclidean Revelations

The eventual development of non-Euclidean geometries by mathematicians such as Gauss, Lobachevsky, and Bolyai revealed that the fourth angle is not always a right angle. Their work demonstrated that geometries exist where the parallel postulate does not hold, and consequently, the fourth angle of a Lambert quadrilateral behaves differently:

  • In hyperbolic geometry, the fourth angle is acute.
  • In Euclidean geometry, the fourth angle is indeed a right angle.
  • In elliptic geometry, the fourth angle is obtuse.

This understanding fundamentally shifted the landscape of geometry.

Properties Across Geometries

Hyperbolic Geometry

In the context of hyperbolic geometry (where the curvature is negative, often normalized to -1), a Lambert quadrilateral exhibits specific properties. If we denote the vertices as A, O, B, F, with right angles at A, O, and B, the angle at F (∠AFB) is always acute. The lengths of the sides and the angles are related through hyperbolic trigonometric functions.

Explore Hyperbolic Details ➡️

Euclidean Geometry

Within the familiar framework of Euclidean geometry, a Lambert quadrilateral is simply a rectangle. If three angles are right angles (90 degrees), the sum of the interior angles of any quadrilateral is 360 degrees. Therefore, the fourth angle must also be 90 degrees (360 - 90 - 90 - 90 = 90).

Explore Euclidean Details ➡️

Elliptic Geometry

In elliptic geometry (where the curvature is positive), the sum of the angles of a quadrilateral is greater than 360 degrees. Consequently, if a Lambert quadrilateral has three right angles, the fourth angle must be greater than 90 degrees, making it obtuse.

Explore Elliptic Details ➡️

Lambert Quadrilateral in Hyperbolic Geometry

Defining the Figure

Consider a Lambert quadrilateral denoted as AOBF, where the angles ∠FAO, ∠AOB, and ∠OBF are right angles (90 degrees). In hyperbolic geometry, with a constant Gaussian curvature of -1, the fourth angle, ∠AFB, is necessarily acute.

Hyperbolic Trigonometric Relations

The relationships between the sides and angles in such a hyperbolic Lambert quadrilateral are governed by hyperbolic trigonometric identities. Let OA and BF be the lengths of the sides adjacent to the right angles, and OB and AF be the other two sides. Let OF be the diagonal. The following equations hold:


sinh(AF) = sinh(OB) * cosh(BF)
tanh(AF) = cosh(OA) * tanh(OB)
sinh(BF) = sinh(OA) * cosh(AF)
tanh(BF) = cosh(OB) * tanh(OA)
cosh(OF) = cosh(OA) * cosh(AF)
cosh(OF) = cosh(OB) * cosh(BF)
sin(∠AFB) = cosh(OB) / cosh(AF) = cosh(OA) / cosh(BF)
cos(∠AFB) = sinh(OA) * sinh(OB) = tanh(AF) * tanh(BF)
cot(∠AFB) = tanh(OA) * sinh(AF) = tanh(OB) * sinh(BF)
sin(∠AOF) = sinh(AF) / sinh(OF)
cos(∠AOF) = tanh(OA) / tanh(OF)
tan(∠AOF) = tanh(AF) / sinh(OA)

Here, sinh, cosh, and tanh represent the hyperbolic sine, cosine, and tangent functions, respectively. These equations illustrate how the geometry dictates precise relationships between lengths and angles, differing fundamentally from Euclidean geometry.

Lambert Quadrilateral in Euclidean Geometry

The Rectangle

In Euclidean geometry, the sum of the interior angles of any quadrilateral is always 360 degrees. If a quadrilateral has three right angles (90 degrees each), the sum of these three angles is 270 degrees. Therefore, the fourth angle must be 360 - 270 = 90 degrees. This means any Lambert quadrilateral in Euclidean space is, by definition, a rectangle.

Properties

As a rectangle, a Euclidean Lambert quadrilateral possesses all the properties of rectangles: opposite sides are equal in length and parallel, and diagonals bisect each other and are equal in length. This case was the focus of much historical effort to prove the parallel postulate.

Lambert Quadrilateral in Elliptic Geometry

The Obtuse Case

Elliptic geometry, characterized by positive curvature (like the surface of a sphere), behaves differently. On a sphere, for instance, the sum of the angles of any triangle exceeds 180 degrees. Consequently, the sum of the interior angles of a quadrilateral is greater than 360 degrees. If a Lambert quadrilateral in elliptic geometry has three right angles, the fourth angle must necessarily be obtuse (greater than 90 degrees) to satisfy this condition.

Spherical Geometry Example

A common example is found on the surface of a sphere. Consider a quadrilateral formed by:

  • The North Pole (vertex 1).
  • A point on the equator directly south of the North Pole (vertex 2).
  • Another point on the equator 90 degrees of longitude away from vertex 2 (vertex 3).
  • A point on the same meridian as vertex 1 and vertex 3, but located such that the angle at this vertex is 90 degrees (vertex 4).

The angles at the North Pole, vertex 2, and vertex 3 are 90 degrees. The angle at vertex 4 will be obtuse, demonstrating the principle.

Key Mathematical Formulas

Hyperbolic Trigonometry

The precise relationships in hyperbolic geometry are crucial for understanding the nature of the Lambert quadrilateral in this non-Euclidean space. The formulas derived from hyperbolic trigonometry precisely define the interplay between side lengths and angles when three angles are right angles.

For a Lambert quadrilateral AOBF with right angles at A, O, and B, and curvature K = -1:

Side Relationships:

Diagonal Relationships:

Angle Relationships (specifically ∠AFB):

These formulas highlight the non-intuitive relationships governing lengths and angles in hyperbolic space, where the standard Euclidean rules do not apply.

Illustrative Examples

Orbifold Fundamental Domains

Lambert quadrilaterals serve as fundamental domains in certain symmetry groups, particularly in hyperbolic geometry. These domains tile the hyperbolic plane, reflecting the symmetries of the space.

The source material references specific orbifolds related to Lambert quadrilaterals:

  • Orbifold *p222: This symmetry group can utilize a Lambert quadrilateral as its fundamental domain. For instance, a domain with a 60-degree angle at one corner (related to the fourth angle of the quadrilateral) can define a tiling with *3222 symmetry.
  • Orbifold *4222: Similarly, a fundamental domain with a 45-degree angle can correspond to a tiling with *4222 symmetry.
  • Limiting Case: The limiting Lambert quadrilateral, possessing three right angles and a fourth angle approaching zero degrees, defines an ideal vertex at infinity. This configuration relates to *∞222 symmetry.

These examples illustrate how the geometric properties of the Lambert quadrilateral are fundamental to understanding the structure and symmetry of hyperbolic spaces.

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References

References

A full list of references for this article are available at the Lambert quadrilateral Wikipedia page

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