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From the Beginning to Plato

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144 PYTHAGOREANS AND ELEATICS<br />

against a very slow one. The slow runner is given a start. The stretch covered by<br />

<strong>the</strong> faster runner is divided up in such a way that it appears <strong>the</strong> faster can never<br />

catch <strong>the</strong> slower within any finite time. This drives home <strong>the</strong> point that speed is<br />

irrelevant. No limit of speed is prescribed or needed by <strong>the</strong> argument; <strong>the</strong> speed<br />

of <strong>the</strong> fast runner could increase without limit without removing <strong>the</strong> problem.<br />

(c)<br />

The ‘Arrow’<br />

Ano<strong>the</strong>r way of looking at things supposedly in motion throughout a time-stretch<br />

is <strong>to</strong> select any one moment during that stretch. Say an arrow is in flight.<br />

1 At any one moment <strong>the</strong> arrow must be ‘in one place’. No part of it can be in<br />

two places at once; so it must occupy ‘a space equal <strong>to</strong> itself (i.e. of <strong>the</strong> same<br />

shape and size).<br />

2 The arrow must be at rest at this moment. There is no distance through<br />

which it moves, in a moment; hence it does not move at a moment, so it<br />

must be at rest at that moment.<br />

3 But <strong>the</strong> moment chosen was an arbitrary moment during <strong>the</strong> flight of <strong>the</strong><br />

arrow. It follows that <strong>the</strong> arrow must be at rest at all moments during its<br />

flight.<br />

4 Hence, since <strong>the</strong> arrow during its flight is never not at a moment of its flight,<br />

<strong>the</strong> arrow is always at rest during its flight; so it never moves during its flight.<br />

The above argument cannot claim <strong>to</strong> be more than a plausible filling-out of<br />

Aris<strong>to</strong>tle’s abbreviated report (Physics VI 9, 239b5–9 and 30–3). 41 Aris<strong>to</strong>tle<br />

himself is interested only in step (4), where he thinks <strong>to</strong> find <strong>the</strong> fallacy; he gives<br />

<strong>the</strong> only briefest sketch of (1), (2) and (3). 42<br />

(d)<br />

The ‘Moving Rows’<br />

Aris<strong>to</strong>tle (Physics VI 9, 239b33–240a18) reports this argument in terms of<br />

unspecified ‘masses’ on a racecourse; <strong>to</strong> make it easier for a modern reader, <strong>the</strong><br />

masses may be thought of as railway trains. 43<br />

Consider three railway trains of <strong>the</strong> same length, on three parallel tracks. One<br />

of <strong>the</strong> trains is moving in <strong>the</strong> ‘up’ direction, ano<strong>the</strong>r is moving at <strong>the</strong> same speed<br />

in <strong>the</strong> ‘down’ direction, and <strong>the</strong> third is stationary. As may be easily verified,<br />

ei<strong>the</strong>r of <strong>the</strong> moving trains takes twice as long <strong>to</strong> pass <strong>the</strong> stationary train as it<br />

does <strong>to</strong> pass <strong>the</strong> o<strong>the</strong>r moving train.<br />

Just how Zeno derived a contradiction from this fact, is uncertain. According<br />

<strong>to</strong> Aris<strong>to</strong>tle, Zeno simply assumed that <strong>the</strong> passing-times must be equal, since <strong>the</strong><br />

speeds are equal and <strong>the</strong> two masses passed are equal in length. Then it follows<br />

that <strong>the</strong> time is equal <strong>to</strong> twice itself. The assumption, though, has often been

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