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Villarceau Circles


TorusCircles
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Villarceau circles are the oblique circles lying on a ring torus (Villarceau 1848, Schmidt 1950, Coxeter 1969, Melzak 1983). Exactly four distinct circles lying entirely on a ring torus pass through each point P. Two are familiar: the circle in a plane parallel to the equatorial plane and the circle in a plane through the axis of the torus. The other two are Villarceau circles.

The assertion that there are exactly four, rather than merely at least four, was proved by Blum (1980). Takeuchi (2000, Proposition 4.2(i), p. 128) states this result explicitly and attributes it to Blum. In the notation below, the ring torus condition is c>a>0.

Sym (2009, p. 1) discusses the historical connection with Darboux and states that a complete sufficiently smooth surface with exactly four circles through each point must be a standard torus, citing Takeuchi (2000). This characterization is incorrect as stated. Inversion of a ring torus about an inversion center off its surface gives a compact smooth ring cyclide and preserves circles and their incidence (De Comité 2015). Applying the inverse inversion shows that there are still exactly four circles through each point. Such a ring cyclide need not be a surface of revolution, so the four-circle property does not characterize a standard torus.

To see that two additional circles exist, consider a coordinate system with origin at the center of torus, with z^^ pointing up. Specify the position of P by its angle phi measured around the tube of the torus. Define phi=0 for the circle of points farthest away from the center of the torus (i.e., the points with x^2+y^2=R^2), and draw the x-axis as the intersection of a plane through the z-axis and passing through P with the xy-plane. Rotate about the y-axis by an angle theta, where

 theta=sin^(-1)(a/c).
(1)

In terms of the old coordinates, the new coordinates are

x=x_1costheta-z_1sintheta
(2)
z=x_1sintheta+z_1costheta.
(3)

So in (x_1,y_1,z_1) coordinates, the equation of the torus becomes

 [sqrt((x_1costheta-z_1sintheta)^2+y_1^2)-c]^2+(x_1sintheta+z_1costheta)^2=a^2.
(4)

Expanding the left side gives

 (x_1costheta-z_1sintheta)^2+y_1^2+c^2
 -2csqrt((x_1costheta-z_1sintheta)^2+y_1^2)+(x_1sintheta+z_1costheta)^2=a^2.
(5)

But

 (x_1costheta-z_1sintheta)^2+(x_1sintheta+z_1costheta)^2=x_1^2+z_1^2,
(6)

so

 x_1^2+y_1^2+z_1^2+c^2-2csqrt((x_1costheta-z_1sintheta)^2+y_1^2)=a^2.
(7)

In the z_1=0 plane, plugging in (1) and factoring gives

 [x_1^2+(y_1-a)^2-c^2][x_1^2+(y_1+a)^2-c^2]=0.
(8)

This gives the circles

 x_1^2+(y_1-a)^2=c^2
(9)

and

 x_1^2+(y_1+a)^2=c^2
(10)

in the z_1 plane. Written in matrix form with parameter t in [0,2pi), these are

C_1=[ccost; csint+a; 0]
(11)
C_2=[ccost; csint-a; 0].
(12)

In the original (x,y,z) coordinates,

C_1=[costheta 0 -sintheta; 0 1 0; -sintheta 0 costheta][ccost; csint+a; 0]
(13)
=[ccosthetacost; csint+a; -csinthetacost]
(14)
C_2=[costheta 0 sintheta; 0 1 0; -sintheta 0 costheta][ccost; csint-a; 0]
(15)
=[ccosthetacost; csint-a; -csinthetacost].
(16)

The point P must satisfy

 z=asinphi=csinthetacost,
(17)

so

 cost=(asinphi)/(csintheta).
(18)

Plugging this in for x_1 and y_1 gives the angle psi by which the circle must be rotated about the z-axis in order to make it pass through P,

 psi=tan^(-1)(y/x)=(csint+a)/(ccosthetacost)=(csqrt(1-cos^2t)+a)/(ccosthetacost).
(19)

The four circles passing through P are therefore

C_1=[cospsi sinpsi 0; -sinpsi cospsi 0; 0 0 1][ccosthetacost; csint+a; -csinthetacost]
(20)
C_2=[cospsi sinpsi 0; -sinpsi cospsi 0; 0 0 1][ccosthetacost; csint-a; -csinthetacost]
(21)
C_3=[(c+acosphi)cost; (c+acosphi)sint; asinphi]
(22)
C_4=[c+acost; 0; asint].
(23)

See also

Ring Cyclide, Ring Torus, Standard Tori, Torus

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References

Blum, R. "Circles on Surfaces in the Euclidean 3-Space." In Geometry and Differential Geometry (Ed. R. Artzy and I. Vaisman). Lecture Notes in Mathematics, Vol. 792. Berlin, Germany: Springer-Verlag, pp. 213-221, 1980. https://doi.org/10.1007/BFb0088679.Coxeter, H. S. M. Introduction to Geometry, 2nd ed. New York: Wiley, pp. 132-133, 1969.De Comité, F. "Yvon-Villarceau Circle Equivalents on Dupin Cyclides." In Proceedings of Bridges 2015: Mathematics, Music, Art, Architecture, Culture (Ed. K. Delp, C. S. Kaplan, D. McKenna, and R. Sarhangi). Phoenix, AZ: Tessellations Publishing, pp. 253-258, 2015. https://archive.bridgesmathart.org/2015/bridges2015-253.html.Kabai, S. Mathematical Graphics I: Lessons in Computer Graphics Using Mathematica. Püspökladány, Hungary: Uniconstant, p. 125, 2002.Melzak, Z. A. Invitation to Geometry. New York: Wiley, pp. 63-72, 1983.Schmidt, H. Die Inversion und ihre Anwendungen. Munich, Germany: Oldenbourg, 1950.Sym, A. "Darboux's Greatest Love." J. Phys. A: Math. Theor. 42, 404001, 2009. https://doi.org/10.1088/1751-8113/42/40/404001.Takeuchi, N. "Cyclides." Hokkaido Math. J. 29, 119-148, 2000. https://doi.org/10.14492/hokmj/1350912960.Villarceau, M. "Théorème sur le tore." Nouv. Ann. Math. 7, 345-347, 1848.

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Villarceau Circles

Cite this as:

Weisstein, Eric W. "Villarceau Circles." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/VillarceauCircles.html

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