Turns spacing on a toroid, works when the number of turns is small (so you aren't filling it out, there's room to move) and the permeability is low (which is the case for RF mixes like #2, less so for #52, very little for ferrite as in CMCs/transformers).
Key observation: the fields around the wires do not change when a core is introduced. The field from any given turn overlaps the field from each other, and with them being so far apart, they don't cancel out until, well, comparable distances away. So, there is considerable leakage, on the order of 1/mu_r of the total.
Which means we can manipulate that leakage, by scrunching the turns together to raise self-inductance (and increase external field, approximating more closely a short solenoid).
So, expect a tuning range on the order of 1/mu_r times the nominal / total.
There's also a solenoidal component, axial with the toroid: consider if the thickness of the toroid were reduced to zero, so that the helix of the winding is reduced to zero. Now you have a single turn, going around the toroid's center line: a loop with field parallel to the toroid['s axis of rotational symmetry]. This is reduced if the winding doubles back on itself (which is less preferable for RF purposes, due to interlayer capacitance and proximity effect), or returning the winding end along the core (without winding more turns along the way).
Tim