In algebraic geometry, the first polar, or simply polar of an algebraic plane curve C of degree n with respect to a point Q is an algebraic curve of degree n−1 which contains every point of C whose tangent line passes through Q. It is used to investigate the relationship between the curve and its dual, for example in the derivation of the Plücker formulas.
Let C be defined in homogeneous coordinates by f(x, y, z) = 0 where f is a homogeneous polynomial of degree n, and let the homogeneous coordinates of Q be (a, b, c). Define the operator
\DeltaQ=a{\partial\over\partialx}+b{\partial\over\partialy}+c{\partial\over\partialz}.
If P=(p, q, r) is a non-singular point on the curve C then the equation of the tangent at P is
x{\partialf\over\partialx}(p,q,r)+y{\partialf\over\partialy}(p,q,r)+z{\partialf\over\partialz}(p,q,r)=0.
The class of C may be defined as the number of tangents that may be drawn to C from a point not on C (counting multiplicities and including imaginary tangents). Each of these tangents touches C at one of the points of intersection of C and the first polar, and by Bézout's theorem there are at most n(n−1) of these. This puts an upper bound of n(n−1) on the class of a curve of degree n. The class may be computed exactly by counting the number and type of singular points on C (see Plücker formula).
The p-th polar of a C for a natural number p is defined as ΔQpf(x, y, z) = 0. This is a curve of degree n−p. When p is n−1 the p-th polar is a line called the polar line of C with respect to Q. Similarly, when p is n−2 the curve is called the polar conic of C.
Using Taylor series in several variables and exploiting homogeneity, f(λa+μp, λb+μq, λc+μr) can be expanded in two ways as
\munf(p,q,r)+λ\mun-1\DeltaQf(p,q,r)+
1 | |
2 |
λ2\mun-2
2 | |
\Delta | |
Q |
f(p,q,r)+...
λnf(a,b,c)+\muλn-1\DeltaPf(a,b,c)+
1 | |
2 |
\mu2λn-2
2 | |
\Delta | |
P |
f(a,b,c)+....
1 | |
p! |
p | |
\Delta | |
Q |
f(p,q,r)=
1 | |
(n-p)! |
n-p | |
\Delta | |
P |
f(a,b,c).
If the polar line of C with respect to a point Q is a line L, then Q is said to be a pole of L. A given line has (n−1)2 poles (counting multiplicities etc.) where n is the degree of C. To see this, pick two points P and Q on L. The locus of points whose polar lines pass through P is the first polar of P and this is a curve of degree n−1. Similarly, the locus of points whose polar lines pass through Q is the first polar of Q and this is also a curve of degree n−1. The polar line of a point is L if and only if it contains both P and Q, so the poles of L are exactly the points of intersection of the two first polars. By Bézout's theorem these curves have (n−1)2 points of intersection and these are the poles of L.[2]
For a given point Q=(a, b, c), the polar conic is the locus of points P so that Q is on the second polar of P. In other words, the equation of the polar conic is
2 | |
\Delta | |
(x,y,z) |
f(a,b,c)=x2{\partial2f\over\partialx2}(a,b,c)+2xy{\partial2f\over\partialx\partialy}(a,b,c)+...=0.
H(f)=\begin{bmatrix}
\partial2f | |
\partialx2 |
&
\partial2f | |
\partialx\partialy |
&
\partial2f | |
\partialx\partialz |
\ \\
\partial2f | |
\partialy\partialx |
&
\partial2f | |
\partialy2 |
&
\partial2f | |
\partialy\partialz |
\ \\
\partial2f | |
\partialz\partialx |
&
\partial2f | |
\partialz\partialy |
&
\partial2f | |
\partialz2 |
\end{bmatrix},
. Higher Plane Curves. Hodges, Foster, and Figgis. 1879. 49ff.. George Salmon.