hyperbolic surface - significado y definición. Qué es hyperbolic surface
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Qué (quién) es hyperbolic surface - definición

NON-EUCLIDEAN GEOMETRY
Lobachevsky geometry; Lobachevskian or hyperbolic geometry; Hyperbolic plane; Gauss-Bolyai-Lobachevsky space; Lobachevsky plane; Ultraparallel; Knit theory; Lobachevskian geometry; Lobachevski plane; Lobachevskii geometry; Lobachevskii space; Analytic hyperbolic geometry; Bolyai-Lobachevskian geometry; Bolyai geometry; Bolyai surface; Bolyai-Lobachevskian surface; Hyperbolic Geometry; Gauss–Bolyai–Lobachevsky space; Models of the hyperbolic plane; Lobachevskian; Lobachevsky-Bolyai-Gauss Geometry; Ultraparallel line; Hyperbolic plane (geometry); Hemisphere model; Hyperbolic surface; Gans model; History of hyperbolic geometry; Ultra-parallel
  • A collection of crocheted hyperbolic planes, in imitation of a coral reef, by the [[Institute For Figuring]]
  • Lines through a given point ''P'' and asymptotic to line ''R''
  • Lines through a given point ''P'' and asymptotic to line ''R''.
  • An [[apeirogon]] and circumscribed [[horocycle]] in the [[Poincare disk model]]
  • Hypercycle and pseudogon in the [[Poincare disk model]]
  • Poincaré disk model with [[truncated triheptagonal tiling]]
  • A triangle immersed in a saddle-shape plane (a [[hyperbolic paraboloid]]), along with two diverging ultra-parallel lines
  • The "hyperbolic soccerball" is a paper model which approximates (part of) the hyperbolic plane as a [[truncated icosahedron]] approximates the sphere.
  • Poincaré disk, hemispherical and hyperboloid models are related by [[stereographic projection]] from −1. [[Beltrami–Klein model]] is [[orthographic projection]] from hemispherical model. [[Poincaré half-plane model]] here projected from the hemispherical model by rays from left end of Poincaré disk model.
  • [[Rhombitriheptagonal tiling]] of the hyperbolic plane, seen in the [[Poincaré disk model]]

Hyperbolic trajectory         
  • gravitational potential well]] of the central mass shows potential energy, and the kinetic energy of the hyperbolic trajectory is shown in red. The height of the kinetic energy decreases as the speed decreases and distance increases according to Kepler's laws. The part of the kinetic energy that remains above zero total energy is that associated with the hyperbolic excess velocity.
  • Hyperbolic trajectories followed by objects approaching central object (small dot) with same hyperbolic excess velocity (and semi-major axis (=1)) and from same direction but with different impact parameters and eccentricities. The yellow line indeed passes around the central dot, approaching it closely.
TRAJECTORY OF ANY OBJECT AROUND A CENTRAL BODY WITH MORE THAN ENOUGH SPEED TO ESCAPE THE CENTRAL OBJECT'S GRAVITATIONAL PULL
Hyperbolic orbit; Hyperbolic Orbit; Hyperbolic excess velocity; Radial hyperbolic trajectory; Radial hyperbolic orbit
In astrodynamics or celestial mechanics, a hyperbolic trajectory is the trajectory of any object around a central body with more than enough speed to escape the central object's gravitational pull. The name derives from the fact that according to Newtonian theory such an orbit has the shape of a hyperbola.
Hyperbolic space         
  • E<sup>3</sup>]]''
HOMOGENEOUS SPACE THAT HAS A CONSTANT NEGATIVE CURVATURE (NOT ANY HYPERBOLIC MANIFOLD)
Hyperbolic 3-space; Real hyperbolic space; Hyperbolic Space; Hyperbolic spaces; Hyperbolic Spaces; H^n
In mathematics, hyperbolic space of dimension n is the unique simply connected, n-dimensional Riemannian manifold of constant sectional curvature equal to -1. It is homogeneous, and satisfies the stronger property of being a symmetric space.
Hyperbolic geometry         
In mathematics, hyperbolic geometry (also called Lobachevskian geometry or Bolyai–Lobachevskian geometry) is a non-Euclidean geometry. The parallel postulate of Euclidean geometry is replaced with:

Wikipedia

Hyperbolic geometry

In mathematics, hyperbolic geometry (also called Lobachevskian geometry or Bolyai–Lobachevskian geometry) is a non-Euclidean geometry. The parallel postulate of Euclidean geometry is replaced with:

For any given line R and point P not on R, in the plane containing both line R and point P there are at least two distinct lines through P that do not intersect R.

(Compare the above with Playfair's axiom, the modern version of Euclid's parallel postulate.)

The hyperbolic plane is a plane where every point is a saddle point. Hyperbolic plane geometry is also the geometry of pseudospherical surfaces, surfaces with a constant negative Gaussian curvature. Saddle surfaces have negative Gaussian curvature in at least some regions, where they locally resemble the hyperbolic plane.

A modern use of hyperbolic geometry is in the theory of special relativity, particularly the Minkowski model.

When geometers first realised they were working with something other than the standard Euclidean geometry, they described their geometry under many different names; Felix Klein finally gave the subject the name hyperbolic geometry to include it in the now rarely used sequence elliptic geometry (spherical geometry), parabolic geometry (Euclidean geometry), and hyperbolic geometry. In the former Soviet Union, it is commonly called Lobachevskian geometry, named after one of its discoverers, the Russian geometer Nikolai Lobachevsky.

This page is mainly about the 2-dimensional (planar) hyperbolic geometry and the differences and similarities between Euclidean and hyperbolic geometry. See hyperbolic space for more information on hyperbolic geometry extended to three and more dimensions.