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Soddy's hexlet - Wikipedia, the free encyclopedia

Soddy's hexlet

From Wikipedia, the free encyclopedia

Soddy's hexlet is a theorem about mutually tangent spheres published by Frederick Soddy in 1937[1], and is the three-dimensional analog of the problem of Apollonius.[2] Given three mutually tangent spheres (denoted A, B, and C), it is always possible to find a chain of six other spheres (S1-S6, the "hexlet") that are tangent to the three original spheres and successively tangent to each other. For example, sphere S3 is tangent to A, B, and C, and also to spheres S2 and S4. The chain of spheres closes perfectly; for example, sphere S6 is tangent to spheres S5 and also to S1. Even more surprisingly, Soddy showed that there are an infinite number of such hexlets for a given set of three original spheres.

A Dupin cyclide. It is fairly easy to imagine a 1-parameter family of spheres inside this "tube". The tube is also the envelope of a 1-parameter family of spheres touching it (in circles) from the outside. This outer family is harder to visualize and includes two planes, which are "spheres through infinity".
A Dupin cyclide. It is fairly easy to imagine a 1-parameter family of spheres inside this "tube". The tube is also the envelope of a 1-parameter family of spheres touching it (in circles) from the outside. This outer family is harder to visualize and includes two planes, which are "spheres through infinity".

The envelope of Soddy's hexlets is a Dupin cyclide, an inversion of the torus. Thus Soddy's construction shows that a cyclide of Dupin is the envelope of a 1-parameter family of spheres in two different ways, and each sphere in either family is tangent to two spheres in same family and three spheres in the other family[3]. This result was probably known to Charles Dupin, who discovered the cyclides that bear his name in his 1803 dissertation[4] under Gaspard Monge.

Interestingly, Soddy's hexlet was also derived independently in Japan, as shown by Sangaku tablets from 1822 in the Kanagawa prefecture.[5]

Contents

[edit] Simple proof by inversion

Soddy's hexlet theorem can be proved most readily by geometric inversion, which transforms spheres into spheres or into planes (which can be regarded as spheres of infinite radius). If the center of inversion lies on the sphere itself, the sphere is transformed into a plane; otherwise, it is transformed into another sphere.

Inversion in the point of tangency between spheres A and C transforms them into parallel planes, which may be denoted as a and c. Since sphere B is tangent to both A and C and since tangency is not affected by inversion, B must be transformed into another sphere b of radius r that is tangent to both planes; hence, b is sandwiched between the two planes a and c. Six balls (s1-s6) of the same radius r may be packed around b and also sandwiched between the bounding planes a and c, just as six pennies may be packed around a single penny on a table. Re-inversion restores the three original spheres, and transforms the six surrounding balls into the six spheres of Soddy's hexlet, S1-S6, which generally have different radii.

An infinite variety of hexlets may be generated by rotating the six balls s1-s6 in their plane by an arbitrary angle before re-inverting them. The envelope produced by such rotations is the torus that surrounds the sphere b and is sandwiched between the two planes a and c; thus, the torus has an inner radius r and outer radius 3r. After the re-inversion, this torus becomes a cyclide.

[edit] See also

[edit] References

  1. ^ Soddy, Frederick (1937). "The bowl of integers and the hexlet". Nature, London 139: 77-79. 
  2. ^ Ogilvy, CS (1990). Excursions in Geometry. Dover. ISBN 0-486-26530-7. 
  3. ^ Coxeter, HSM (1952). "Interlocked rings of spheres". Scripta Math 18: 113-121. 
  4. ^ Entry in MacTutor History of Mathematics
  5. ^ Rothman, T (1998). "Japanese Temple Geometry". Scientific American 278: 85–91. 

[edit] External links

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