Why the ancients argued about the arrow and not the sling
Correction, 2026-09-18, to the first version of this note. It claimed the sling is missing from ancient philosophical argument. That is wrong, and the exception is important: Plutarch, De facie in orbe lunae 923C, has the moon “saved from falling by its very motion and the rapidity of its revolution, just as missiles placed in slings are kept from falling by being whirled around in a circle”. That is Newton’s apparatus on Newton’s case, and the Classical Scholia name Plutarch among the ancients Newton credited with the doctrine of gravitation, so it was available in a text he was mining while writing the propositions it models. Section 4 below treats it. What survives of the original claim is that the exception stayed isolated, and that the reason it did is the one this note gives.
The ancient debate on motion is otherwise almost entirely rectilinear. Zeno’s arrow, the Vaiśeṣika arrow, Vasubandhu’s denial of passage, Hui Shi’s stick and the Mohist shadow all take straight-line or static cases, while the sling and stone, which is where Newton defines centripetal force, does almost no work in the philosophical argument even though slings were ordinary objects. The pattern holds, and the reason is that the ancient question and Newton’s are at different rungs of the same ladder: the ancients asked whether motion is possible at all, which is a first-order question about succession, and Newton asked what sustains a departure from straight-line motion, which is second order and becomes askable only once inertia is assumed. Section 3 gives the one ancient case that is genuinely circular, the whirled firebrand, and shows it was used for a third purpose again: neither possibility nor force, but the difference between what appears and what is. Lateral to the main argument; no ledger promotion.
1. Newton’s definition uses the sling
Definition V of the Principia introduces the concept with the stone, in the Motte translation held in this repository:
A stone, whirled about in a sling, endeavours to recede from the hand that turns it; and by that endeavour, distends the sling, and that with so much the greater force, as it is revolved with the greater velocity, and as soon as ever it is let go, flies away. That force which opposes itself to this endeavour, and by which the sling perpetually draws back the stone towards the hand, and retains it in its orbit, because it is directed to the hand as the centre of the orbit, I call the centripetal force.
The sentence before it names the planets, “perpetually drawn aside from the rectilinear motions, which otherwise they would pursue”. So the sling is the laboratory model of Proposition I, and the clause “which otherwise they would pursue” is the load-bearing one: the straight line is what happens by default, and only the deviation needs a cause.
2. The ladder, and why the ancients stood on its first rung
Theorem 5 of the paper makes the difference exact. For a signal that is an \(n\)-th order departure, with the lower orders unknown and therefore nuisance, the quantity bounded below is \(m\,(P^{(n)})^2\,\tau^{2n-1}\gtrsim\kappa\):
| Rung | Question | Nuisance | Bound |
|---|---|---|---|
| \(n=1\) | Is it moving at all? | position | \(mv^2\tau\ge8z^2\kappa\) |
| \(n=2\) | Is a force acting? | position and velocity | \(F^2\tau^3/m\ge18z^2\kappa\) |
Zeno, the Vaiśeṣika sūtras and Vasubandhu are all at \(n=1\): the thing in dispute is whether the arrow moves, and the unknown to be beaten is merely where it is. The sling is at \(n=2\), and so is Galileo’s comparison and all of Newton’s Book I. The second rung cannot even be stated without treating uniform motion as needing no account, because otherwise curved motion is not more puzzling than straight motion and there is no distinguished thing for a centripetal force to explain. Ancient physics on the whole treats rest as the natural state, so the second rung is not available to it, and the case that would exhibit it has no work to do.
The Vaiśeṣika comes closest to opening it. VS 5.1.17 gives impulsion the first motion only and hands the rest to the impression the previous motion deposits, so the continuation of motion is already not being charged to a continuing push. What is missing is the further step that a straight continuation is free while a curved one is not, and without that step the sling is an ordinary event rather than a problem.
3. The one circular case, used for a third purpose
Indian sources do have a whirled object: the firebrand circle, alātacakra, the ring of fire seen when a burning stick is swung. Vasubandhu uses it in the Abhidharmakośabhāṣya, Pradhan 189.23–24, arguing that because contact with the parts is successive, the cognition of a whole is really a cognition of the parts, avayaveṣv eva tad-buddhir alātacakravat, “the awareness is of the parts only, as with the firebrand circle”. At Pradhan 33.9 the same image appears with āśuvṛttyā, “by rapid action”, in asking whether the eye grasps objects of its own size. The firebrand is therefore an argument about sampling: a rapid succession presents itself as a continuous extended thing, and the continuity is the observer’s.
That is a third use, and for this programme it is the most interesting of the three. It is the ancient form of the point Theorem 5 makes about records rather than about the world: below the mesh a succession is indistinguishable from the continuous object it mimics, and above it the succession is recoverable. The Buddhist example runs the inference in the direction the theorem does not license, from the appearance being a succession to the whole being unreal, but the phenomenon it names is exactly the one being measured.
4. Plutarch’s sling, and why it stayed isolated
The companion records the passage and its limits. Two points bear on the argument here.
The inference runs opposite to Newton’s. For Plutarch the whirling is what prevents the fall, so rapid revolution supplies a sustaining effect and weight is overcome; for Newton the cord pulls the stone inward, and what the pull diverts is the straight line the stone would otherwise keep. The same object supports both readings, and what decides between them is which motion is held to need no cause. Plutarch’s next clause, at 923D, that “each thing is governed by its natural motion unless it be diverted by something else”, comes close to the principle that decides it, with natural motion still doing the work inertia later does; and because for a heavenly body the natural motion was circular, the clause does not yield Newton’s reading.
That is why the example stayed isolated rather than starting a tradition. Used inside a physics where circular motion is natural for the heavens and rest natural below, the sling illustrates a conclusion already reached rather than posing a problem. It becomes a problem only at the second rung, where uniform straight motion is free and any departure is owed to a cause, and the step to that rung was not taken. Aristotle’s De caelo I.2 is the reason on the celestial side, and is cited here at metadata level only.
5. Consequence for STATE
The case selection in the ancient sources is explained rather than merely noted: the arrow is the first rung and the sling the second, and the second needs inertia before it becomes a question. The Vaiśeṣika impression is the nearest ancient approach to the missing premise. The firebrand supplies the one circular example and uses it for sampling, which is the closest ancient statement of what Theorem 5 says about records. Section 7 of the paper now carries the point in short form.
Open: whether any Greek source besides Plutarch argues about the sling rather than merely using it, with Ps.-Aristotle Mechanica and Aristotle Physics VIII.10 on projectiles as the places to look; and whether the alātacakra appears in the Nyāya-Vaiśeṣika commentaries on VS 5.1.16 beside the arrow and the bird, which the Upaskāra is reported to do and this collection cannot yet check.