Separation of bounded Schwarz--Christoffel sides #
Two nonadjacent bounded sides of a Schwarz--Christoffel polygon can be separated by following
either of the two boundary arcs between them. Polygon.ShortTurn treats the direct arc when its
directions turn through less than π. This file treats the complementary arc through the vertex
at infinity when the direct turn is at least π. The closing condition makes its two unbounded
pieces point in the same direction, and the complementary turn is at most π.
Combining the two cases shows that every pair of nonadjacent bounded sides is disjoint under the
classical convex-polygon hypotheses: strictly ordered prevertices, exponents in (-1, 0), and
total exponent -2. These lemmas supply the bounded-side part of the global
boundary-simplicity argument.
Main results #
TauCeti.im_exp_neg_mul_schwarzChristoffelVertex_sub_pos_of_long_turnputs the chord along the complementary boundary arc strictly to one side of the later bounded edge.TauCeti.disjoint_schwarzChristoffelPolygon_edgeSet_of_long_turnseparates nonadjacent bounded sides when their direct turn is at leastπ.TauCeti.disjoint_schwarzChristoffelPolygon_bounded_edgeSetseparates every pair of nonadjacent bounded sides.
References #
- L. Ahlfors, Complex Analysis, Ch. 6, Section 2.
- T. Driscoll and L. Trefethen, Schwarz--Christoffel Mapping, Ch. 2.
After rotating by -θ, the height of a bounded Schwarz--Christoffel side vector is its length
times the sine of its edge angle measured from θ.
If the direct turn from bounded side i to bounded side j is at least π, the chord from
the end of side j to the start of side i, following the complementary boundary arc through
infinity, lies strictly to the left of side j.
The index condition leaves at least one complete bounded side on the direct arc. The exponent
conditions make all edge directions strictly ordered through one full turn, while the total
exponent -2 identifies the two unbounded pieces as a single positive-direction closing side.
Two nonadjacent bounded Schwarz--Christoffel sides are disjoint when their direct edge-angle
turn is at least π. The separating chord follows the complementary boundary arc through the
vertex at infinity, whose turn is at most π.
Under the classical convex Schwarz--Christoffel hypotheses, every two nonadjacent bounded
sides are disjoint. The proof uses the direct boundary arc when its turn is less than π and
the complementary arc through infinity otherwise.