The drawn component is an unknot. Its exterior is a solid torus , in which is a pattern of a satellite knot. A meridian of a solid torus of is , whereas its longitudinal direction is . Thus the prescribed gluing sends these directions to and , respectively. This identifies with a tubular neighborhood of with its zero Seifert framing.
Removing the pattern before making this identification gives
Equivalently, meridionally filling the remaining boundary first removes from the construction and leaves ; its filling core is the required satellite knot .
In the original link diagram, the two parallel passages through a meridional disk of run in the same direction; closing them uses a single interchange. The winding number of a satellite pattern is therefore two. Untwisting the surrounding disk shows that is the unknot (the pattern is the cable knot, up to the harmless sign of its single interchange). In particular . The Satellite formula for the Alexander polynomial now gives the concise answer
Here allows multiplication by . Reversing the winding orientation replaces by , giving the same Alexander polynomial of a knot up to such a unit.
Take the untwisted Whitehead double of a trefoil knot. The Whitehead pattern has winding number of a satellite pattern zero and becomes the unknot when its companion is the unknot. The Satellite formula for the Alexander polynomial therefore gives
The Whitehead pattern is geometrically essential in its solid torus, so the satellite knot with nontrivial companion is nontrivial. Hence is not isotopic to the unknot despite having trivial Alexander polynomial of a knot.
Let contain the pattern of a satellite knot . Its class in is the winding number of a satellite pattern. Winding number zero therefore makes null-homologous in , so bounds an oriented embedded surface . Let
For any companion knot , an embedding as a tubular neighborhood of carries to a Seifert surface for the satellite knot . Hence
and the bound depends only on the pattern.
In an irreducible three-manifold with incompressible boundary, a minimizing surface can be cut along a separating incompressible torus after removing inessential intersection circles. The essential pieces have no disk or sphere components, so their costs add. Minimizing independently in the pieces and gluing their matching boundary curves gives the corresponding upper bound. This allows Thurston norm calculations for satellite knots.