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From the Beginning to Plato

From the Beginning to Plato

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The Arguments about Motion<br />

FROM THE BEGINNING TO PLATO 143<br />

(a)<br />

Aris<strong>to</strong>tle’s evidence<br />

There is only one certain primary source for <strong>the</strong> content of Zeno’s arguments<br />

about motion: Aris<strong>to</strong>tle, who states and discusses <strong>the</strong>m in Physics VI and VIII (VI<br />

2, 233a21–30; VI 9, 239b5–240a18; VIII 8, 263a4–b9). Aris<strong>to</strong>tle’s source is not<br />

known; no book of Zeno that might have contained <strong>the</strong>m is recorded. It is<br />

perfectly possible that <strong>the</strong>y reached Aris<strong>to</strong>tle by oral tradition. In any case, while<br />

<strong>the</strong>re is no reason <strong>to</strong> doubt that <strong>the</strong>y are substantially au<strong>the</strong>ntic, <strong>the</strong>re is also no<br />

reason <strong>to</strong> suppose that Zeno’s own formulations have been faithfully preserved.<br />

(A source possibly independent of Aris<strong>to</strong>tle is mentioned in (d) below.)<br />

The four individual arguments, as Aris<strong>to</strong>tle reports <strong>the</strong>m, derive contradictions<br />

from <strong>the</strong> supposition that something moves. Three of <strong>the</strong>m purport <strong>to</strong> show that<br />

what moves, does not move. They are ‘dramatized’, in so far as <strong>the</strong>y introduce<br />

particular supposed moving things: a runner; two runners; an arrow; three<br />

moving and stationary masses. Aris<strong>to</strong>tle presents <strong>the</strong> arguments as designed <strong>to</strong> be<br />

mutually independent. 38<br />

(b)<br />

The ‘Stadium’ and <strong>the</strong> ‘Achilles’<br />

Suppose a runner is <strong>to</strong> run along a running-track. The stretch <strong>to</strong> be traversed (call<br />

it S) may be considered as divided up in<strong>to</strong> substretches in various ways. Given <strong>the</strong><br />

starting and finishing points we understand what is meant by ‘<strong>the</strong> first half of S’,<br />

‘<strong>the</strong> third quarter of S’ and so on. It seems that however short a substretch is<br />

specified in this way, it will always have positive length and may be thought of<br />

as divided in<strong>to</strong> two halves. 39<br />

Going on in this way we can specify a division of S in<strong>to</strong> substretches which<br />

will be such that <strong>the</strong> runner runs through a well-ordered but infinite series of<br />

substretches. First <strong>the</strong> runner traverses <strong>the</strong> first half, <strong>the</strong>n half of what remains,<br />

<strong>the</strong>n half of what remains, and so on. In this way, for any positive integer n, at<br />

<strong>the</strong> end of <strong>the</strong> nth substretch <strong>the</strong> runner has covered<br />

of S, and <strong>the</strong> nth substretch is ½n of <strong>the</strong> whole length of <strong>the</strong> track. However large a finite number n becomes, <strong>the</strong><br />

fraction is never equal <strong>to</strong> 1; <strong>the</strong>re are infinitely many substretches.<br />

With such a division, <strong>the</strong> series of substretches is well-ordered, and <strong>the</strong> runner<br />

who traverses S has been through all of <strong>the</strong> substretches in order: for every finite<br />

number N, <strong>the</strong> runner has traversed <strong>the</strong> Nth substretch. Hence <strong>the</strong> runner has<br />

traversed an infinite series of substretches, in a finite time; but this is impossible.<br />

This is an expansion of Aris<strong>to</strong>tle’s formulations (Physics VI 2, 233a21–23; VI<br />

9, 239b11–14) of <strong>the</strong> ‘Stadium’ argument. 40 The ‘Achilles’ (Physics VI 9,<br />

239b14–29) makes <strong>the</strong> same point more dramatically, pitting a very fast runner

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