The gap that grows
No packing criterion singles out the golden angle at a fixed head size. That is a genuine result and it leaves an obvious question: what does distinguish it, and why does the pattern collapse at rational angles?
The answer is about growth rather than about a contest.
What the measurement shows
Take the largest circumradius in the triangulation of a head — the biggest empty patch — and measure it in units of the mean spacing, so the answer does not simply shrink as the head fills.
For 135°, which is exactly three-eighths of a turn, the gap grows from 3.1 at two hundred primordia to 9.1 at sixteen hundred. It is not converging; it is growing, and it grows because the pattern has eight radial rows and the wedges between them get wider in proportion as the head gets larger.
For the golden angle it stays between about 0.7 and 0.9 across the same range. So does 137.3°, and so does 106.5°.
The distinction the measurement makes is therefore not golden-versus-everything. It is rational versus irrational, and it is sharp.
Why rational angles fail
If the divergence angle is p/q of a turn, then every qth primordium lands on exactly the same ray from the centre. The pattern has q radial rows and nothing between them.
As the head grows, the rows extend and the wedges between them widen in proportion. There is no mechanism by which anything fills them, because nothing is ever placed at an angle that is not one of the q rays.
That is complete collapse rather than degradation, and it happens at every rational angle, including ones very close to the golden angle. The failure is discontinuous in a way that a contest at fixed n cannot show.
Why irrational angles do not
The multiples of an irrational number, taken modulo one, are equidistributed — they fill the circle, and no gap survives forever.
There is a sharper statement, the three-distance theorem, which says that the first n multiples of any irrational divide the circle into intervals of at most three distinct lengths. That is a strong regularity, it holds for every irrational, and it is why any irrational angle produces a lattice that keeps filling.
How well it fills depends on how badly the number is approximated by rationals: a number with a very good rational approximation at some denominator behaves almost like that rational for a while, producing near-rows that persist until the head grows past them. That is what makes 137.0° look poor at moderate size while remaining bounded in the limit.
The claim in its correct form
Putting the three pieces together gives the version that survives.
Rational angles fail completely — gaps grow without bound, at every rational.
Every irrational angle works in the sense that gaps stay bounded.
How quickly it starts working depends on how well the angle is approximated by rationals, and the golden angle is the extreme case: it is the number for which those approximations are worst, so its lattice is the one that never has a bad phase at any scale.
That last clause is what “optimal” should mean here, and it is a statement about arithmetic rather than about geometry. It has a precise form, it is a theorem, and it is considerably more interesting than the packing story it usually gets flattened into.
What this means for a plant
Rather less than the claim implies, and it is worth being clear.
A plant does not need the extreme case. Any angle comfortably away from a simple fraction produces a pattern with bounded gaps, and the difference between the golden angle and a merely-irrational neighbour is invisible in a head of a few hundred primordia.
What a plant does need is to avoid the rationals, and the dynamical model explains why it does: a rule that places each element away from its neighbours is under continuous pressure away from any angle whose multiples pile up, and the golden angle is where that pressure has nowhere left to push.
So the biology does not require the theorem. The theorem explains why the attractor is where it is.