Wolfram Demonstrations Project

This Demonstration shows the relationship between the principal curvatures of a surface and the differential

of the unit normal of the surface. The differential

at a point may be viewed as a linear transformation of the tangent plane at the point, since the derivative of the unit normal is orthogonal to the normal. The eigenvalues of

are the negatives of the principal curvatures of the surface at the point, and correspondingly the eigenvectors are the principal directions. At a point

one may rotate an orthogonal basis for the tangent plane to diagonalize the matrix for

by aligning the basis with the principal directions. One may see how a small tangent vector

is mapped by

and compare it to the actual difference in the normals at the points

and

The lines that are drawn on the surface are lines of curvature, which are curves whose tangents at every point match one of the principal directions.

Contributed by: Michael Rogers (Oxford College of Emory University)

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In addition to the principal curvatures of a surface, this Demonstration illustrates geometrically several interesting concepts: differentials and local linear approximation, linear transformations, eigenvectors and eigenvalues, the orthogonal diagonalization of symmetric matrices, and the relation of the rotation of the normal vector of a surface to the curvature. Note the negative of

is called the shape operator.

To explore

as a linear transformation: move

to a desired location. Move

to change the tangent vector at

; the motion of

may be constrained to move horizontally or vertically. The image vector

is drawn in the plane at the end of the normal at

. The image plane may be drawn with the same basis as the tangent plane (the "reference" grid) or with the image of the basis under

(the "image" grid). The basis of the tangent plane may be rotated with the slider. By rotating the basis to align with the principal directions, the matrix of

may be diagonalized. In the display, numerical values of

, and

are given with respect to the basis of the tangent plane.

The display: the lines on the surface show the principal configuration (lines of curvature). At the point

, the unit normal vector is drawn in black, and the lines of curvature through

are drawn on the surface. For the point

, the normal is drawn twice in green, both at

and at

. There are two things to observe: the angle between the normals and the displacement between the tips of the normals. On the one hand, if the change

is parallel to a principal direction, then the angle rotated will be approximately the negative of the curvature times the distance moved; on the other hand, the displacement will be approximately equal to

. Basis vectors are highlighted in the tangent plane and the image grid.

Umbilic points are points where the normal curvature is the same in all directions and

is scalar. Some of them are bookmarked in the + menu in the upper left. Darboux first classified curvature umbilics into three types, now sometimes called lemons, stars, and monstars (or lemonstars). For more information, see G. Darboux, "Note VII: Sur la forme des lignes de courbure dans la voisinage d'un ombilic," Leçons sur la Théorie Générale des Surfaces, Vol. 4, Paris: Gauthier–Villars, 1896 pp. 448–465.

Questions for exploration:

When the matrix of

is diagonalized, the image grid is a rectangle. Why?

When the vector

is rotated, which way does its image rotate? When is it in the same direction and when is it different? Is it ever the case that the image of

does not rotate but changes length?

Sometimes the tip of the image vector

stays close to the tip of the green normal based at

, and sometimes it does not. Why? To clarify: since the normal vectors are unit length, the green vector rotates away from the plane. One expects the tips to lie on a line approximately parallel to the normal. In other words, if the viewpoint is adjusted so the reference grids align, one tip should be on top of the other. Sometimes they are closer, and sometimes not.