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A history of Greek mathematics - Wilbourhall.org

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;<br />

;<br />

94 ARCHIMEDES<br />

method attributed to him by Vitruvius, 1<br />

namely by measuring<br />

successively the volumes <strong>of</strong> fluid displaced by three equal<br />

weights, (1) the crown, (2) an equal weight <strong>of</strong> gold, (3) an<br />

equal weight <strong>of</strong> silver respectively. Suppose, as before, that<br />

the weight <strong>of</strong> the crown is W and that it contains weights<br />

tu 1<br />

and iv 2<br />

<strong>of</strong> gold and silver respectively. Then<br />

(1) the crown displaces a certain volume <strong>of</strong> the fluid, V, say<br />

;<br />

(2) the weight W <strong>of</strong> gold displaces a volume V v say, <strong>of</strong> the<br />

fluid<br />

therefore a weight w x<br />

<strong>of</strong> gold displaces a volume yiy- V x<br />

<strong>of</strong><br />

the fluid<br />

(3) the weight W <strong>of</strong> silver displaces V 2<br />

,<br />

say, <strong>of</strong> the fluid;<br />

w<br />

therefore a weight w 2<br />

<strong>of</strong> silver displaces —• V 2<br />

.<br />

It follows that V = ^<br />

•<br />

V 1<br />

+ ^<br />

• V<br />

2<br />

,<br />

whence we derive (since W = w 1<br />

+ w 2 )<br />

y\ v 2<br />

-v<br />

w ~<br />

2<br />

V-V]'<br />

the latter ratio being obviously equal to that obtained by the<br />

other method.<br />

The last propositions (8 and 9) <strong>of</strong> Book I deal with the case<br />

<strong>of</strong> any segment <strong>of</strong> a sphere lighter than a fluid and immersed<br />

in it in such a way that either (1) the curved surface is downwards<br />

and the base is entirely outside the fluid, or (2) the<br />

curved surface is upwards and the base is entirely submerged,<br />

and it is proved that in either case the segment is in stable<br />

equilibrium when the axis is vertical.<br />

This is expressed here<br />

and in the corresponding propositions <strong>of</strong> Book II by saying<br />

that, ' if the figure be forced into such a position that the base<br />

<strong>of</strong> the segment touches the fluid (at one point), the figure will<br />

not remain inclined but will return to the upright position '.<br />

Book II, which investigates fully the conditions <strong>of</strong> stability<br />

<strong>of</strong> a right segment <strong>of</strong> a paraboloid <strong>of</strong> revolution floating in<br />

a fluid for different values <strong>of</strong> the specific gravity and different<br />

ratios between the axis or height <strong>of</strong> the segment and the<br />

1<br />

De architectural, ix. 3.

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