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Duality (projective geometry)

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Duality in the projective plane refers to the interchangeability between points and lines which preserves incidence properties.

Notice that both points and lines can be represented (on a plane) by means of ordered pairs. A point is represented by the ordered pair (x,y), where x is the abscissa and y is the ordinate, which together are coordinates of the point. A line can likewise be represented by an ordered pair (m,b) where m is the slope and b is the y-intercept.

Given three points

these three points are collinear iff their coordinates satisfy the equation
.
Likewise, given three lines
one can verify that these three lines are concurrent iff their parameters satisfy the equation
Equations (1) and (2) are equivalent to each other up to an exchange of x with m and y with b. Therefore there exists is a way to exchange lines with points in such a way that concurrency is exchanged with collinearity.

It is possible to distinguish lines from points by conjugating ordered pairs. That is, let line (m,b) be represented instead by its conjugate Then it can be verified that the intersection L1.L2 of a pair of lines L1 and L2 is

where b1 and b2 are negative y-intercepts. Also, the common line P1.P2 passing through a pair of points P1 and P2 is
Equation (4) can be seen to be the same as equation (3), after exchanging m with x and b with y, and applying the following rules of conjugation:

Indeed, if equation (3) is represented as
then applying rule (6) yields
Applying rule (7) then yields
and applying rule (5) finally yields
which is equation (4).

Thus it is possible to imagine a pair of planes S1 and S2, and a bijective relation between loci of points in the two planes, such that points in S2 correspond to lines in S1, and points in S1 correspond to lines in S2.

One way to establish such bijection is to model the projective plane, not as an extended affine plane, but as a "unit sphere modulo antipodes", i.e. a unit sphere in which antipodal points are equivalent. Then through points P1 and P2 in S1 passes a line L3 which is actually a great circle. But to these two original points correspond a pair of great circles L1 and L2 in S2, such that if S2 and S1 are superposed, then L1 is the unique great circle in a plane perpendicular to the line through the pair of points P1, and L2 is the unique great circle in a plane perpendicular to the line through the pair of points P2. These great circles L1 and L2 intersect at a pair of points P3 in S2. The line through P3 is the cross product of the lines through P1 and P2. Then the unique great circle perpendicular to point P3 is line L3 in S1.

Therefore to every great circle in S1 corresponds a unique pair of points (which are actually the same point) in S2, such that if S1 and S2 are superposed, then the line passing through the pair of points is perpendicular to the great circle. The above sentence remains true if S1 and S2 are exchanged. This establishes the bijective nature of the duality in the projective plane.

It must be noted that in the "unit sphere modulo antipodes", one "line", i.e. great circle, must be chosen to be the line at infinity. This line may be chosen to be the equator by convention.

There is also a duality in projective 3-space, in which points correspond to planes, and lines correspond to lines. This is analogous to duality of polyhedra in solid geometry, where points are dual to faces, and sides are dual to sides, so that the icosahedron is dual to the dodecahedron, and the cube is dual to the octahedron.