Hyperboloid: Difference between revisions

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Undid revision 1296180660 by 174.208.225.57 (talk) – unexplained
 
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\end{array} \right)
\end{array} \right)
</math>
</math>
 
* For <math>d>0</math> one obtains a hyperboloid of one sheet,  
*For <math>d>0</math> one obtains a hyperboloid of one sheet,  
* For <math>d<0</math> a hyperboloid of two sheets, and  
*For <math>d<0</math> a hyperboloid of two sheets, and  
* For <math>d=0</math> a double cone.
*For <math>d=0</math> a double cone.


One can obtain a parametric representation of a hyperboloid with a different coordinate axis as the axis of symmetry by shuffling the position of the <math>c s</math> term to the appropriate component in the equation above.
One can obtain a parametric representation of a hyperboloid with a different coordinate axis as the axis of symmetry by shuffling the position of the <math>c s</math> term to the appropriate component in the equation above.


===Generalised equations===
=== Generalised equations ===
More generally, an arbitrarily oriented hyperboloid, centered at {{math|'''v'''}}, is defined by the equation
More generally, an arbitrarily oriented hyperboloid, centered at {{math|'''v'''}}, is defined by the equation
<math display="block">(\mathbf{x}-\mathbf{v})^\mathrm{T} A (\mathbf{x}-\mathbf{v}) = 1,</math>
<math display="block">(\mathbf{x}-\mathbf{v})^\mathrm{T} A (\mathbf{x}-\mathbf{v}) = 1,</math>
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If the hyperboloid has the equation
If the hyperboloid has the equation
<math> {x^2 \over a^2} + {y^2 \over b^2} - {z^2 \over c^2}= 1</math>  then the lines
<math> {x^2 \over a^2} + {y^2 \over b^2} - {z^2 \over c^2}= 1</math>  then the lines
<math display="block">g^{\pm}_{\alpha}:
<math display="block">g^{\pm}_{\alpha}:
  \mathbf{x}(t) = \begin{pmatrix} a\cos\alpha \\ b\sin\alpha \\ 0\end{pmatrix}
  \mathbf{x}(t) = \begin{pmatrix} a\cos\alpha \\ b\sin\alpha \\ 0\end{pmatrix}
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==== Plane sections ====
==== Plane sections ====
For simplicity the plane sections of the ''unit hyperboloid'' with equation <math> \ H_1: x^2+y^2-z^2=1</math> are considered. Because a hyperboloid in general position is an affine image of the unit hyperboloid, the result applies to the general case, too.
For simplicity the plane sections of the ''unit hyperboloid'' with equation <math> \ H_1: x^2+y^2-z^2=1</math> are considered. Because a hyperboloid in general position is an affine image of the unit hyperboloid, the result applies to the general case, too.
 
* A plane with a slope less than 1 (1 is the slope of the lines on the hyperboloid) intersects <math>H_1</math> in an ''ellipse'',
*A plane with a slope less than 1 (1 is the slope of the lines on the hyperboloid) intersects <math>H_1</math> in an ''ellipse'',
* A plane with a slope equal to 1 containing the origin intersects <math>H_1</math> in a ''pair of parallel lines'',
*A plane with a slope equal to 1 containing the origin intersects <math>H_1</math> in a ''pair of parallel lines'',
* A plane with a slope equal 1 not containing the origin intersects <math>H_1</math> in a ''parabola'',
*A plane with a slope equal 1 not containing the origin intersects <math>H_1</math> in a ''parabola'',
* A tangential plane intersects <math>H_1</math> in a ''pair of intersecting lines'',
*A tangential plane intersects <math>H_1</math> in a ''pair of intersecting lines'',
* A non-tangential plane with a slope greater than 1 intersects <math>H_1</math> in a ''hyperbola''.<ref>[http://www.mathematik.tu-darmstadt.de/~ehartmann/cdg-skript-1998.pdf CDKG: Computerunterstützte Darstellende und Konstruktive Geometrie (TU Darmstadt)] (PDF; 3,4&nbsp;MB), S. 116</ref>
*A non-tangential plane with a slope greater than 1 intersects <math>H_1</math> in a ''hyperbola''.<ref>[http://www.mathematik.tu-darmstadt.de/~ehartmann/cdg-skript-1998.pdf CDKG: Computerunterstützte Darstellende und Konstruktive Geometrie (TU Darmstadt)] (PDF; 3,4&nbsp;MB), S. 116</ref>
Obviously, any one-sheet hyperboloid of revolution contains circles. This is also true, but less obvious, in the general case (see [[circular section]]).
Obviously, any one-sheet hyperboloid of revolution contains circles. This is also true, but less obvious, in the general case (see [[circular section]]).


=== Hyperboloid of two sheets {{anchor|Two sheets}}===
=== Hyperboloid of two sheets <span class="anchor" id="Two sheets"></span> ===
[[File:Hyperboloid-2s.svg|thumb|hyperboloid of two sheets: generation by rotating a hyperbola]]
[[File:Hyperboloid-2s.svg|thumb|hyperboloid of two sheets: generation by rotating a hyperbola]]
[[File:Hyperbo-2s-ca.svg|thumb|hyperboloid of two sheets: plane sections]]
[[File:Hyperbo-2s-ca.svg|thumb|hyperboloid of two sheets: plane sections]]
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<math display="block">H_2: \ x^2+y^2-z^2 = -1.</math>
<math display="block">H_2: \ x^2+y^2-z^2 = -1.</math>
which can be generated by a rotating [[hyperbola]] around one of its axes (the one that cuts the hyperbola)
which can be generated by a rotating [[hyperbola]] around one of its axes (the one that cuts the hyperbola)
 
* A plane with slope less than 1 (1 is the slope of the asymptotes of the generating hyperbola) intersects <math>H_2</math> either in an ''ellipse'' or in a ''point'' or not at all,
*A plane with slope less than 1 (1 is the slope of the asymptotes of the generating hyperbola) intersects <math>H_2</math> either in an ''ellipse'' or in a ''point'' or not at all,
* A plane with slope equal to 1 containing the origin (midpoint of the hyperboloid) does ''not intersect'' <math>H_2</math>,
*A plane with slope equal to 1 containing the origin (midpoint of the hyperboloid) does ''not intersect'' <math>H_2</math>,
* A plane with slope equal to 1 not containing the origin intersects <math>H_2</math> in a ''parabola'',  
*A plane with slope equal to 1 not containing the origin intersects <math>H_2</math> in a ''parabola'',  
* A plane with slope greater than 1 intersects <math>H_2</math> in a ''hyperbola''.<ref>[http://www.mathematik.tu-darmstadt.de/~ehartmann/cdg-skript-1998.pdf CDKG: Computerunterstützte Darstellende und Konstruktive Geometrie (TU Darmstadt)] (PDF; 3,4&nbsp;MB), S. 122</ref>
*A plane with slope greater than 1 intersects <math>H_2</math> in a ''hyperbola''.<ref>[http://www.mathematik.tu-darmstadt.de/~ehartmann/cdg-skript-1998.pdf CDKG: Computerunterstützte Darstellende und Konstruktive Geometrie (TU Darmstadt)] (PDF; 3,4&nbsp;MB), S. 122</ref>
Obviously, any two-sheet hyperboloid of revolution contains circles. This is also true, but less obvious, in the general case (see [[circular section]]).
Obviously, any two-sheet hyperboloid of revolution contains circles. This is also true, but less obvious, in the general case (see [[circular section]]).


''Remark:'' A hyperboloid of two sheets is ''projectively'' equivalent to a sphere.
''Remark'': A hyperboloid of two sheets is ''projectively'' equivalent to a sphere.


===Other properties===
=== Other properties ===


==== Symmetries ====
==== Symmetries ====
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<math display="block">\frac{x^2}{a^2} + \frac{y^2}{b^2} - \frac{z^2}{c^2} = 1 , \quad \frac{x^2}{a^2} + \frac{y^2}{b^2} - \frac{z^2}{c^2} = -1 </math>
<math display="block">\frac{x^2}{a^2} + \frac{y^2}{b^2} - \frac{z^2}{c^2} = 1 , \quad \frac{x^2}{a^2} + \frac{y^2}{b^2} - \frac{z^2}{c^2} = -1 </math>
are
are
*''pointsymmetric'' to the origin,
* ''pointsymmetric'' to the origin,
*''symmetric to the coordinate planes'' and
* ''symmetric to the coordinate planes'' and
*''rotational symmetric'' to the z-axis and symmetric to any plane containing the z-axis, in case of <math>a=b</math> (hyperboloid of revolution).
* ''rotational symmetric'' to the z-axis and symmetric to any plane containing the z-axis, in case of <math>a=b</math> (hyperboloid of revolution).


==== Curvature ====
==== Curvature ====
Whereas the [[Gaussian curvature]] of a hyperboloid of one sheet is negative, that of a two-sheet hyperboloid is positive. In spite of its positive curvature, the hyperboloid of two sheets with another suitably chosen metric can also be used as a [[Hyperboloid model|model]] for hyperbolic geometry.
Whereas the [[Gaussian curvature]] of a hyperboloid of one sheet is negative, that of a two-sheet hyperboloid is positive. In spite of its positive curvature, the hyperboloid of two sheets with another suitably chosen metric can also be used as a [[Hyperboloid model|model]] for hyperbolic geometry.


==In more than three dimensions==
== In more than three dimensions ==
Imaginary hyperboloids are frequently found in mathematics of higher dimensions. For example, in a [[pseudo-Euclidean space]] one has the use of a [[quadratic form]]:
Hyperboloids are frequently found in mathematics of higher dimensions. For example, in a [[pseudo-Euclidean space]] one has the use of a [[quadratic form]]:
<math display="block">q(x) = \left(x_1^2+\cdots + x_k^2\right)-\left(x_{k+1}^2+\cdots + x_n^2\right), \quad k < n .</math>  
<math display="block">q(x) = \left(x_1^2+\cdots + x_k^2\right)-\left(x_{k+1}^2+\cdots + x_n^2\right), \quad k < n .</math>  
When {{math|''c''}} is any [[constant (mathematics)|constant]], then the part of the space given by
When {{math|''c''}} is any [[constant (mathematics)|constant]], then the part of the space given by
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<blockquote>... the velocity vectors always lie on a surface which Minkowski calls a four-dimensional hyperboloid since, expressed in terms of purely real coordinates {{math|(''y''<sub>1</sub>, ..., ''y''<sub>4</sub>)}}, its equation is {{math|''y''{{su|b=1|p=2}} + ''y''{{su|b=2|p=2}} + ''y''{{su|b=3|p=2}} − ''y''{{su|b=4|p=2}} {{=}} −1}}, analogous to the hyperboloid {{math|''y''{{su|b=1|p=2}} + ''y''{{su|b=2|p=2}} − ''y''{{su|b=3|p=2}} {{=}} −1}} of three-dimensional space.{{refn|Minkowski used the term "four-dimensional hyperboloid" only once, in a posthumously-published typescript and this was non-standard usage, as Minkowski's hyperboloid is a three-dimensional submanifold of a four-dimensional Minkowski space <math>M^4.</math><ref>{{Citation|author=Walter, Scott A.| year=1999 | contribution=The non-Euclidean style of Minkowskian relativity|editor=J. Gray|title=The Symbolic Universe: Geometry and Physics 1890-1930|pages=91–127|publisher=Oxford University Press|contribution-url=http://scottwalter.free.fr/papers/1999-symbuniv-walter.html}}</ref>}}</blockquote>
<blockquote>... the velocity vectors always lie on a surface which Minkowski calls a four-dimensional hyperboloid since, expressed in terms of purely real coordinates {{math|(''y''<sub>1</sub>, ..., ''y''<sub>4</sub>)}}, its equation is {{math|''y''{{su|b=1|p=2}} + ''y''{{su|b=2|p=2}} + ''y''{{su|b=3|p=2}} − ''y''{{su|b=4|p=2}} {{=}} −1}}, analogous to the hyperboloid {{math|''y''{{su|b=1|p=2}} + ''y''{{su|b=2|p=2}} − ''y''{{su|b=3|p=2}} {{=}} −1}} of three-dimensional space.{{refn|Minkowski used the term "four-dimensional hyperboloid" only once, in a posthumously-published typescript and this was non-standard usage, as Minkowski's hyperboloid is a three-dimensional submanifold of a four-dimensional Minkowski space <math>M^4.</math><ref>{{Citation|author=Walter, Scott A.| year=1999 | contribution=The non-Euclidean style of Minkowskian relativity|editor=J. Gray|title=The Symbolic Universe: Geometry and Physics 1890-1930|pages=91–127|publisher=Oxford University Press|contribution-url=http://scottwalter.free.fr/papers/1999-symbuniv-walter.html}}</ref>}}</blockquote>


However, the term '''quasi-sphere''' is also used in this context since the sphere and hyperboloid have some commonality (See {{section link||Relation to the sphere}} below).
However, the term '''quasi-sphere''' is also used in this context since the sphere and hyperboloid have some commonality (See ''{{section link||Relation to the sphere}}'' below).


== Hyperboloid structures ==
== Hyperboloid structures ==
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  Killesberg Tower.jpg|The [[Killesberg Tower|Killesberg]] observation tower, [[Stuttgart]], [[Germany]], 2001.
  Killesberg Tower.jpg|The [[Killesberg Tower|Killesberg]] observation tower, [[Stuttgart]], [[Germany]], 2001.
  BMW-Welt at night 2.JPG|[[BMW Welt]], (BMW World), museum and event venue, [[Munich]], [[Germany]], 2007.
  BMW-Welt at night 2.JPG|[[BMW Welt]], (BMW World), museum and event venue, [[Munich]], [[Germany]], 2007.
  Canton tower in asian games opening ceremony.jpg|The [[Canton Tower]], [[China]], 2009.
  Canton tower in asian games opening ceremony.jpg|The [[Canton Tower]], [[China]], 2010.
  Les Essarts-le-Roi Château d'eau.JPG|The [[Essarts-le-Roi]] water tower, [[France]].
  Les Essarts-le-Roi Château d'eau.JPG|The [[Essarts-le-Roi]] water tower, [[France]].
</gallery>
</gallery>


==Relation to the sphere==
== Relation to the sphere ==
In 1853 [[William Rowan Hamilton]] published his ''Lectures on Quaternions'' which included presentation of [[biquaternion]]s.  The following passage from page 673 shows how Hamilton uses biquaternion algebra and vectors from [[quaternion]]s to produce hyperboloids from the equation of a [[sphere]]:
In 1853 [[William Rowan Hamilton]] published his ''Lectures on Quaternions'' which included presentation of [[biquaternion]]s.  The following passage from page 673 shows how Hamilton uses biquaternion algebra and vectors from [[quaternion]]s to produce hyperboloids from the equation of a [[sphere]]:
<blockquote>... the ''equation of the unit sphere'' {{math|1=''ρ''<sup>2</sup> + 1 = 0}}, and change the vector {{math|''ρ''}} to a ''bivector form'', such as {{math|''σ'' + ''τ'' {{radic|−1}}}}.  The equation of the sphere then breaks up into the system of the two following,
<blockquote>... the ''equation of the unit sphere'' {{math|1=''ρ''<sup>2</sup> + 1 = 0}}, and change the vector {{math|''ρ''}} to a ''bivector form'', such as {{math|''σ'' + ''τ'' {{radic|−1}}}}.  The equation of the sphere then breaks up into the system of the two following,
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In the theory of [[quadratic form]]s, a '''unit [[quasi-sphere]]''' is the subset of a quadratic space {{math|''X''}} consisting of the {{math|''x'' &isin; ''X''}} such that the quadratic norm of {{math|''x''}} is one.<ref>[[Ian R. Porteous]] (1995) ''Clifford Algebras and the Classical Groups'', pages 22, 24 & 106, [[Cambridge University Press]] {{ISBN|0-521-55177-3}}</ref>
In the theory of [[quadratic form]]s, a '''unit [[quasi-sphere]]''' is the subset of a quadratic space {{math|''X''}} consisting of the {{math|''x'' &isin; ''X''}} such that the quadratic norm of {{math|''x''}} is one.<ref>[[Ian R. Porteous]] (1995) ''Clifford Algebras and the Classical Groups'', pages 22, 24 & 106, [[Cambridge University Press]] {{ISBN|0-521-55177-3}}</ref>


==See also==
== See also ==
* [[List of surfaces]]
* [[List of surfaces]]
* [[Ellipsoid]]
* [[Ellipsoid]]
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* [[Light cone]]
* [[Light cone]]


==References==
== References ==
{{Reflist}}
{{reflist}}
{{refbegin}}
{{refbegin}}
* [[Wilhelm Blaschke]] (1948) ''Analytische Geometrie'', Kapital V: "Quadriken", Wolfenbutteler Verlagsanstalt.
* [[Wilhelm Blaschke]] (1948) ''Analytische Geometrie'', Kapital V: "Quadriken", Wolfenbutteler Verlagsanstalt.
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{{Commons category|Hyperboloid}}
{{Commons category|Hyperboloid}}


==External links==
== External links ==
{{wiktionary | hyperboloid}}
{{wiktionary | hyperboloid}}
*{{MathWorld |title=Hyperboloid |urlname=Hyperboloid}}
* {{MathWorld |title=Hyperboloid |urlname=Hyperboloid}}
** {{mathworld |urlname=One-SheetedHyperboloid |title=One-sheeted hyperboloid}}
** {{mathworld |urlname=One-SheetedHyperboloid |title=One-sheeted hyperboloid}}
** {{mathworld |urlname=Two-SheetedHyperboloid |title=Two-sheeted hyperboloid}}
** {{mathworld |urlname=Two-SheetedHyperboloid |title=Two-sheeted hyperboloid}}
**{{MathWorld |title=Elliptic Hyperboloid |urlname=EllipticHyperboloid}}
** {{MathWorld |title=Elliptic Hyperboloid |urlname=EllipticHyperboloid}}


[[Category:Geometric shapes]]
[[Category:Geometric shapes]]

Latest revision as of 12:43, 16 July 2025

Template:Short description Script error: No such module "Distinguish".

File:Hyperboloid1.png
Hyperboloid of one sheet
File:DoubleCone.png
conical surface in between
File:Hyperboloid2.png
Hyperboloid of two sheets

In geometry, a hyperboloid of revolution, sometimes called a circular hyperboloid, is the surface generated by rotating a hyperbola around one of its principal axes. A hyperboloid is the surface obtained from a hyperboloid of revolution by deforming it by means of directional scalings, or more generally, of an affine transformation.

A hyperboloid is a quadric surface, that is, a surface defined as the zero set of a polynomial of degree two in three variables. Among quadric surfaces, a hyperboloid is characterized by not being a cone or a cylinder, having a center of symmetry, and intersecting many planes into hyperbolas. A hyperboloid has three pairwise perpendicular axes of symmetry, and three pairwise perpendicular planes of symmetry.

Given a hyperboloid, one can choose a Cartesian coordinate system such that the hyperboloid is defined by one of the following equations: x2a2+y2b2z2c2=1, or x2a2+y2b2z2c2=1. The coordinate axes are axes of symmetry of the hyperboloid and the origin is the center of symmetry of the hyperboloid. In any case, the hyperboloid is asymptotic to the cone of the equations: x2a2+y2b2z2c2=0.

One has a hyperboloid of revolution if and only if a2=b2. Otherwise, the axes are uniquely defined (up to the exchange of the x-axis and the y-axis).

There are two kinds of hyperboloids. In the first case (Template:Math in the right-hand side of the equation): a one-sheet hyperboloid, also called a hyperbolic hyperboloid. It is a connected surface, which has a negative Gaussian curvature at every point. This implies near every point the intersection of the hyperboloid and its tangent plane at the point consists of two branches of curve that have distinct tangents at the point. In the case of the one-sheet hyperboloid, these branches of curves are lines and thus the one-sheet hyperboloid is a doubly ruled surface.

In the second case (Template:Math in the right-hand side of the equation): a two-sheet hyperboloid, also called an elliptic hyperboloid. The surface has two connected components and a positive Gaussian curvature at every point. The surface is convex in the sense that the tangent plane at every point intersects the surface only in this point.

Parametric representations

File:Cylinder - hyperboloid - cone.gif
Animation of a hyperboloid of revolution

Cartesian coordinates for the hyperboloids can be defined, similar to spherical coordinates, keeping the azimuth angle Template:Math, but changing inclination Template:Math into hyperbolic trigonometric functions:

One-surface hyperboloid: Template:Math x=acoshvcosθy=bcoshvsinθz=csinhv

Two-surface hyperboloid: Template:Math x=asinhvcosθy=bsinhvsinθz=±ccoshv

File:Hyperboloid-1s.svg
hyperboloid of one sheet: generation by a rotating hyperbola (top) and line (bottom: red or blue)
File:Hyperbo-1s-cut-all.svg
hyperboloid of one sheet: plane sections

The following parametric representation includes hyperboloids of one sheet, two sheets, and their common boundary cone, each with the z-axis as the axis of symmetry: 𝐱(s,t)=(as2+dcostbs2+dsintcs)

  • For d>0 one obtains a hyperboloid of one sheet,
  • For d<0 a hyperboloid of two sheets, and
  • For d=0 a double cone.

One can obtain a parametric representation of a hyperboloid with a different coordinate axis as the axis of symmetry by shuffling the position of the cs term to the appropriate component in the equation above.

Generalised equations

More generally, an arbitrarily oriented hyperboloid, centered at Template:Math, is defined by the equation (𝐱𝐯)TA(𝐱𝐯)=1, where Template:Math is a matrix and Template:Math, Template:Math are vectors.

The eigenvectors of Template:Math define the principal directions of the hyperboloid and the eigenvalues of A are the reciprocals of the squares of the semi-axes: 1/a2, 1/b2 and 1/c2. The one-sheet hyperboloid has two positive eigenvalues and one negative eigenvalue. The two-sheet hyperboloid has one positive eigenvalue and two negative eigenvalues.

Properties

Hyperboloid of one sheet

Lines on the surface

If the hyperboloid has the equation x2a2+y2b2z2c2=1 then the lines gα±:𝐱(t)=(acosαbsinα0)+t(asinαbcosα±c) ,t, 0α2π  are contained in the surface.

In case a=b the hyperboloid is a surface of revolution and can be generated by rotating one of the two lines g0+ or g0, which are skew to the rotation axis (see picture). This property is called Wren's theorem.[1] The more common generation of a one-sheet hyperboloid of revolution is rotating a hyperbola around its semi-minor axis (see picture; rotating the hyperbola around its other axis gives a two-sheet hyperbola of revolution).

A hyperboloid of one sheet is projectively equivalent to a hyperbolic paraboloid.

Plane sections

For simplicity the plane sections of the unit hyperboloid with equation  H1:x2+y2z2=1 are considered. Because a hyperboloid in general position is an affine image of the unit hyperboloid, the result applies to the general case, too.

  • A plane with a slope less than 1 (1 is the slope of the lines on the hyperboloid) intersects H1 in an ellipse,
  • A plane with a slope equal to 1 containing the origin intersects H1 in a pair of parallel lines,
  • A plane with a slope equal 1 not containing the origin intersects H1 in a parabola,
  • A tangential plane intersects H1 in a pair of intersecting lines,
  • A non-tangential plane with a slope greater than 1 intersects H1 in a hyperbola.[2]

Obviously, any one-sheet hyperboloid of revolution contains circles. This is also true, but less obvious, in the general case (see circular section).

Hyperboloid of two sheets

File:Hyperboloid-2s.svg
hyperboloid of two sheets: generation by rotating a hyperbola
File:Hyperbo-2s-ca.svg
hyperboloid of two sheets: plane sections

The hyperboloid of two sheets does not contain lines. The discussion of plane sections can be performed for the unit hyperboloid of two sheets with equation H2: x2+y2z2=1. which can be generated by a rotating hyperbola around one of its axes (the one that cuts the hyperbola)

  • A plane with slope less than 1 (1 is the slope of the asymptotes of the generating hyperbola) intersects H2 either in an ellipse or in a point or not at all,
  • A plane with slope equal to 1 containing the origin (midpoint of the hyperboloid) does not intersect H2,
  • A plane with slope equal to 1 not containing the origin intersects H2 in a parabola,
  • A plane with slope greater than 1 intersects H2 in a hyperbola.[3]

Obviously, any two-sheet hyperboloid of revolution contains circles. This is also true, but less obvious, in the general case (see circular section).

Remark: A hyperboloid of two sheets is projectively equivalent to a sphere.

Other properties

Symmetries

The hyperboloids with equations x2a2+y2b2z2c2=1,x2a2+y2b2z2c2=1 are

  • pointsymmetric to the origin,
  • symmetric to the coordinate planes and
  • rotational symmetric to the z-axis and symmetric to any plane containing the z-axis, in case of a=b (hyperboloid of revolution).

Curvature

Whereas the Gaussian curvature of a hyperboloid of one sheet is negative, that of a two-sheet hyperboloid is positive. In spite of its positive curvature, the hyperboloid of two sheets with another suitably chosen metric can also be used as a model for hyperbolic geometry.

In more than three dimensions

Hyperboloids are frequently found in mathematics of higher dimensions. For example, in a pseudo-Euclidean space one has the use of a quadratic form: q(x)=(x12++xk2)(xk+12++xn2),k<n. When Template:Math is any constant, then the part of the space given by {x : q(x)=c} is called a hyperboloid. The degenerate case corresponds to Template:Math.

As an example, consider the following passage:[4]

... the velocity vectors always lie on a surface which Minkowski calls a four-dimensional hyperboloid since, expressed in terms of purely real coordinates Template:Math, its equation is Template:Math, analogous to the hyperboloid Template:Math of three-dimensional space.Template:Refn

However, the term quasi-sphere is also used in this context since the sphere and hyperboloid have some commonality (See Template:Section link below).

Hyperboloid structures

Script error: No such module "Labelled list hatnote". One-sheeted hyperboloids are used in construction, with the structures called hyperboloid structures. A hyperboloid is a doubly ruled surface; thus, it can be built with straight steel beams, producing a strong structure at a lower cost than other methods. Examples include cooling towers, especially of power stations, and many other structures.

Relation to the sphere

In 1853 William Rowan Hamilton published his Lectures on Quaternions which included presentation of biquaternions. The following passage from page 673 shows how Hamilton uses biquaternion algebra and vectors from quaternions to produce hyperboloids from the equation of a sphere:

... the equation of the unit sphere Template:Math, and change the vector Template:Math to a bivector form, such as Template:Math. The equation of the sphere then breaks up into the system of the two following,

Template:Block indent and suggests our considering Template:Math and Template:Math as two real and rectangular vectors, such that Template:Block indent

Hence it is easy to infer that if we assume Template:Math, where Template:Math is a vector in a given position, the new real vector Template:Math will terminate on the surface of a double-sheeted and equilateral hyperboloid; and that if, on the other hand, we assume Template:Math, then the locus of the extremity of the real vector Template:Math will be an equilateral but single-sheeted hyperboloid. The study of these two hyperboloids is, therefore, in this way connected very simply, through biquaternions, with the study of the sphere; ...

In this passage Template:Math is the operator giving the scalar part of a quaternion, and Template:Math is the "tensor", now called norm, of a quaternion.

A modern view of the unification of the sphere and hyperboloid uses the idea of a conic section as a slice of a quadratic form. Instead of a conical surface, one requires conical hypersurfaces in four-dimensional space with points Template:Math determined by quadratic forms. First consider the conical hypersurface

  • P={p:w2=x2+y2+z2} and
  • Hr={p : w=r}, which is a hyperplane.

Then PHr is the sphere with radius Template:Math. On the other hand, the conical hypersurface Template:Block indent

In the theory of quadratic forms, a unit quasi-sphere is the subset of a quadratic space Template:Math consisting of the Template:Math such that the quadratic norm of Template:Math is one.[5]

See also

References

Template:Reflist Template:Refbegin

Template:Refend Template:Sister project Template:Sister project

External links

Template:Sister project

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  1. K. Strubecker: Vorlesungen der Darstellenden Geometrie. Vandenhoeck & Ruprecht, Göttingen 1967, p. 218
  2. CDKG: Computerunterstützte Darstellende und Konstruktive Geometrie (TU Darmstadt) (PDF; 3,4 MB), S. 116
  3. CDKG: Computerunterstützte Darstellende und Konstruktive Geometrie (TU Darmstadt) (PDF; 3,4 MB), S. 122
  4. Thomas Hawkins (2000) Emergence of the Theory of Lie Groups: an essay in the history of mathematics, 1869—1926, §9.3 "The Mathematization of Physics at Göttingen", see page 340, Springer Template:ISBN
  5. Ian R. Porteous (1995) Clifford Algebras and the Classical Groups, pages 22, 24 & 106, Cambridge University Press Template:ISBN