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REDUCTION OF THE GENERAL EQUATION OF THE SECOND DEGREE TO CANONICAL FORM

Any equation of the second degree

1) f(x, y, z) = ax^{2} + by^{2} + cz^{2} + 2fyz + 2gxz + 2hxy + 2px + 2qy + 2rz + d = 0

can be reduced to one of 17 different canonical forms by a suitable translation and rotation. Each
canonical form represents a quadric surface. Figure 1 shows a quadric surface (an ellipsoid)
along with its canonical coordinate system x_{c}-y_{c}-z_{c} located at some point (x_{0}, y_{0}, z_{0}) in space
(as referred to the X-Y-Z system). Reduction
of a particular second degree equation to
canonical form involves the following steps:

1] Determining the location (x_{0}, y_{0}, z_{0}) of the
origin of the canonical system x_{c}-y_{c}-z_{c} of the
surface.

2] Determining the orientation of the x_{c}-y_{c}-z_{c}
system (as referred to the X-Y-Z system).

3] Determining the expression for our
equation as expressed with respect to the x_{c}-y_{c}-z_{c} system by performing those substitutions
associated with a translation of the X-Y-Z system to the point (x_{0}, y_{0}, z_{0}) and then a rotation to
the orientation to the x_{c}-y_{c}-z_{c} system.

Determining the origin (x_{0}, y_{0}, z_{0}) of the canonical system. How is the point (x_{0}, y_{0}, z_{0}) found?
If the quadratic surface has a center, point (x_{0}, y_{0}, z_{0}) corresponds to a center. A quadric surface
may have a single center, a line of centers, or a plane of centers. If there is more than one center,
translation to any center will do. Of the 17 quadric surfaces , 14 have centers. We compute the
coordinates of a center using the equation

Three surfaces, the elliptic and hyperbolic paraboloids and the parabolic cylinder, do not have
centers. In the case of these three, the point (x_{0}, y_{0}, z_{0}) corresponds to their vertices. The elliptic
and hyperbolic paraboloids have a single vertex and the parabolic cylinder has a line of vertices.
In the case of a line of vertices, translation to any vertex will do. These vertices must be found
by some technique or procedure.

Determining the orientation of the canonical system.
In the problem of translation to the canonical system
origin we have noted that there may not be a single
point that we must translate to but instead we may have
a range of points that we can translate to (as in the case
of a line of centers or a plane of centers). The same
kind of situation exists in the problem of finding the
orientation of the canonical coordinate system. In some
cases there is a range of orientations that we can rotate
to instead of just a single orientation. Consider the
surface of revolution shown in Figure 2. Note that we
can turn the canonical system x_{c}-y_{c}-z_{c} about the z_{c} axis through any angle from 0^{o} to 360^{o} and
there is no change, one position is as good as another, the surface remains in canonical form.
There is a range of acceptable directions for the x axis (and the y axis). This same thing will
occur with any surface of revolution. With any surface of revolution there will exist a plane of
acceptable directions for two of the axes corresponding to a rotation of the system about the third
axis, the axis of symmetry. Now consider the case of a sphere located in space. In this case the
canonical system can have any orientation. No matter how it is oriented the sphere is still in
canonical form. Here we can choose any direction for the x axis and then rotate the system

about
the x axis to point the y axis in any direction we wish to give the system an orientation. Next
question. How do we determine the directions of the x_{c}, y_{c}, and z_{c} axes of the canonical system?
We compute a set of eigenvectors associated with the quadric surface. The directions of the
eigenvectors give the directions of the canonical system axes. In the case of a surface of
revolution where there is a plane of acceptable directions for two of the axes there will be a
corresponding plane of eigenvectors. We arbitrarily pick one eigenvector in the plane for one
axis and one perpendicular to it for the other axis (the eigenvectors radiate out in all directions
from a point).

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