In geometry, a hypercone (or spherical cone) is the figure in the 4-dimensional Euclidean space represented by the equation
x2+y2+z2-w2=0.
It is a quadric surface, and is one of the possible 3-manifolds which are 4-dimensional equivalents of the conical surface in 3 dimensions. It is also named "spherical cone" because its intersections with hyperplanes perpendicular to the w-axis are spheres. A four-dimensional right hypercone can be thought of as a sphere which expands with time, starting its expansion from a single point source, such that the center of the expanding sphere remains fixed. An oblique hypercone would be a sphere which expands with time, again starting its expansion from a point source, but such that the center of the expanding sphere moves with a uniform velocity.
A right spherical hypercone can be described by the function
\vec\sigma(\phi,\theta,t)=(ts\cos\theta\cos\phi,ts\cos\theta\sin\phi,ts\sin\theta,t)
A right spherical hypercone with radius r and height h can be described by the function
\vec\sigma(\phi,\theta,t)=\left(t\cos\phi\sin\theta,t\sin\phi\sin\theta,t\cos\theta,
h | |
r |
t\right)
\vec\sigma(\phi,\theta,t)=(vxt+ts\cos\theta\cos\phi,vyt+ts\cos\theta\sin\phi,vzt+ts\sin\theta,t)
(vx,vy,vz)
Note that the 3D-surfaces above enclose 4D-hypervolumes, which are the 4-cones proper.
The spherical cone consists of two unbounded nappes, which meet at the origin and are the analogues of the nappes of the 3-dimensional conical surface. The upper nappe corresponds with the half with positive w-coordinates, and the lower nappe corresponds with the half with negative w-coordinates.
If it is restricted between the hyperplanes w = 0 and w = r for some nonzero r, then it may be closed by a 3-ball of radius r, centered at (0,0,0,r), so that it bounds a finite 4-dimensional volume. This volume is given by the formula r4, and is the 4-dimensional equivalent of the solid cone. The ball may be thought of as the 'lid' at the base of the 4-dimensional cone's nappe, and the origin becomes its 'apex'.
This shape may be projected into 3-dimensional space in various ways. If projected onto the xyz hyperplane, its image is a ball. If projected onto the xyw, xzw, or yzw hyperplanes, its image is a solid cone. If projected onto an oblique hyperplane, its image is either an ellipsoid or a solid cone with an ellipsoidal base (resembling an ice cream cone). These images are the analogues of the possible images of the solid cone projected to 2 dimensions.
The (half) hypercone may be constructed in a manner analogous to the construction of a 3D cone. A 3D cone may be thought of as the result of stacking progressively smaller discs on top of each other until they taper to a point. Alternatively, a 3D cone may be regarded as the volume swept out by an upright isosceles triangle as it rotates about its base.
A 4D hypercone may be constructed analogously: by stacking progressively smaller balls on top of each other in the 4th direction until they taper to a point, or taking the hypervolume swept out by a tetrahedron standing upright in the 4th direction as it rotates freely about its base in the 3D hyperplane on which it rests.
The hypervolume of a four-dimensional pyramid and cone is
H= | 1 |
4 |
Vh
where V is the volume of the base and h is the height (the distance between the centre of the base and the apex). For a spherical cone with a base volume of , the hypervolume is
H= | 1 | Vh= |
4 |
1 | \left( | |
4 |
4 | |
3 |
\pi
| ||||
r |
\pir3h
The lateral surface volume of a right spherical cone is where
r
l
4 3 \pir3+
4 3 \pir2\sqrt{r2+h2}
(the volume of the base plus the volume of the lateral 3D surface; the term
is the slant height)\sqrt{r2+h2}
4 3 \pir2\left(r+\sqrt{r2+h2}\right)
where
is the radius andr
is the height.h
4 3 \pir3+
4 3 \pir2l
4 3 \pir2\left(r+l\right)
where
is the radius andr
is the slant height.l
1 3 Ar+
1 3 Al
1 3 A\left(r+l\right)
where
is the base surface area,A
is the radius, andr
is the slant height.l
See main article: Minkowski space. If the w-coordinate of the equation of the spherical cone is interpreted as the distance ct, where t is coordinate time and c is the speed of light (a constant), then it is the shape of the light cone in special relativity. In this case, the equation is usually written as:
x2+y2+z2-(ct)2=0,
which is also the equation for spherical wave fronts of light.[1] The upper nappe is then the future light cone and the lower nappe is the past light cone.[2]