Joachimsthal's NotationsFerdinand Joachimsthal (1818-1861) was a German mathematician and educator famous for the high quality of his lectures and the books he wrote. The notations named after him and discussed below serve one of the examples where the language of mathematics is especially auspicious for derivation and memorization of properties of mathematical objects. Joachimsthal's notations have had extended influence beyond the study of second order equations and conic sections, compare for example the work of F. Morley. A general second degree equation
represents a plane conic, or a conic section, i.e., the intersection of a circular two-sided cone with a plane. The equations for ellipses, parabolas, and hyperbolas all can be written in this form. These curves are said to be non-degenerate conics. Non-degenerate conics are obtained when the plane cutting a cone does not pass through its vertex. If the plane does go through the cone's vertex, the intersection may be either two crossing straight lines, a single straight line and even a point. These point sets are said to be degenerate conics. In the following, we shall be only concerned with a non-degenerate case. The left-hand side in (1) will be conveniently denoted as s:
so that the second degree equation (1) acquires a very short form:
A point P(x1, y1) may or may not lie on the conic defined by (1) or (3). If it does, we get an identity by substituting
which has a convenient Joachimsthal's equivalent
For another point P(x2, y2) we similarly define s22 and, in general, for points
Thus, sii = 0 means that P(xi, yi) lies on the conic (3), There is also a mixed notation. For two points P(xi, yi) and
Clearly for P(xi, yi) = P(xj, yj), (7) reduces to (6). An important observation is that sij is symmetrical in its indices:
The last of Joachimsthal's conventions brings the first whiff of an indication as to how useful the notations may be. In sij both
The curious thing about (9) is that, although sij was probably perceived as a number, si appears to dependent on "variable" x and y and thus is mostly perceived as a function of these variables. As a function of x and y, (9) is linear, i.e. of first degree, so that TheoremLet point P(xi, yi) lie on the conic s = 0. In other words, assume that ProofAny point P(x, y) on the line through two distinct points P(x1, y1) and P(x2, y2) is a linear combination of the two points:
which is just a parametric equation of the straight line. Substitute (10) into (2). The exercise may be a little tedious but is quite straightforward. The result is a quadratic expression in t:
Line (10) and conic (1) will have 0, 1, or 2 common points depending on the number of roots of the quadratic equation
The line is tangent to the conic iff the quadratic equation has two equal roots, i.e. when
This is an interesting identity valid for any line tangent to the conic, with
Now, since this is true for any point
which proves the theorem.
Tangent PairIf two points P(x1, y1) and P(x2, y2) are such that the line joining them is tangent to a conic s = 0, then as in (13),
The latter is a quadratic equation which may be factorized into the product of two linear equations each representing a tangent to the conic through ExampleLet s = x2 + 4y2 - 25, so that
So that (16) becomes
Obviously the equation has no real roots (besides
(16) then becomes
First, let's simplify this to
Second, let's multiply out and simplify by collecting the like terms:
which is factorized into
Conclusion: here are two tangents from (5, 5/2) to the ellipse:
Poles and Polars With Respect To a ConicLet P(x1, y1) be a point outside a conic Then the tangents have the equations (15)
and also meet at P(x1, y1):
Because of the symmetry of the notations, we have
which says that points
The latter is uniquely determined by P(x1, y1), which, too, can be retrieved from (20). We define Thus we see that the pole/polar definitions generalize naturally from the circle to other non-degenerate conics. We now prove La Hire's TheoremIf point P(x1, y1) lies on the polar of P(x2, y2) with respect to a conic ProofIneed, P(x1, y1) lies on the polar Beautiful. References
Poles and Polars
Conics
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