The track shape is the race
Every track here is a chute swept along a descending centreline, and all of them share one collision model. What differs is the path: a constant-radius helix, a tightening funnel, a slalom whose axis slides side to side, an oval speedway with two hairpins, an hourglass pinched at the waist.
Those differences decide the character of the race far more than any physics setting. A funnel accelerates the pack and squeezes it together, which produces close finishes. A wide helix lets a fast marble get clear early. A slalom keeps forcing the field across each other, which produces constant position changes and few clean leads.
One constraint runs through all of them: the centreline never goes momentarily vertical, because the chute’s lateral axis is derived from the horizontal perpendicular of the tangent, and a vertical tangent has no defined lateral axis. Every shape is built from a circulation term with a positive lower bound on its radius, which guarantees the chute never twists through itself.

