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FLIPPABLE SURFACE
A flippable surface is a surface globally invariant under the action of a half-turn (or axial symmetry).
A surface with Cartesian equation
can be identified as flippable if their exists a half-turn r of
such that .
With the + sign, the half-turn does not swap the two
faces of the surface; examples:
- all the surfaces
of revolution
- the ellipsoid,
the centered quadrics, and more generally all the surfaces with equation
that are invariant under action of the three half-turns around the axes.
- the cross-cap,
and more generally all the surfaces with equation
that are invariant under the action of the half-turn around Oz.
With the - sign, the half-turn swaps the two faces of the surface; taking the axis of the half-turn to be equal to the line we get a general implicit equation of these surfaces: with ; examples:
- the plane z = 0
- the hyperbolic paraboloid |
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video 1 |
- Plücker's conoid |
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video 2 |
- the symmetric parabolic Dupin cyclide |
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video 3 |
- the surface |
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video 4 |
- Costa's algebraic surface |
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video 5 |
- the surface |
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video 6 |
- the Enneper minimal surfaces, and Costa's minimal surface.
REMARK: all the surfaces of the above box have an equation of the type ; their isometry group is composed of the identity, the half-turn around Oz that does not swap the faces, the two half-turns around , two reflections, and two rotorotations of order 4, this group is isomorphic to that of the isometries of the square.
See more generally the surfaces
with rotational symmetry.
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© Robert FERRÉOL 2017