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A history of Greek mathematics - Wilbourhall.org

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56 ARCHIMEDES<br />

case <strong>of</strong> all, where we are told that 0D l :AD 2 > 349450 :<br />

and then that OD.DA > 591j:153. At the points marked<br />

* and f in the table Archimedes simplifies the ratio a :<br />

2<br />

c and<br />

a :<br />

z<br />

c before calculating b 2<br />

, b z<br />

respectively, by multiplying each<br />

term in the first case by 5 % and in the second case by JJ.<br />

He gives no explanation <strong>of</strong> the exact figure taken as the<br />

approximation to the square root in each case, or <strong>of</strong> the<br />

method by which he obtained it. We may, however, be sure<br />

23409<br />

that the method amounted to the use <strong>of</strong> the formula (a±b) 2<br />

= a 2 + 2 ab + b 2 , much as our method <strong>of</strong> extracting the square<br />

root also depends upon it.<br />

We have already seen (vol. i, p. 232) that, according to<br />

Heron, Archimedes made a still closer approximation to the<br />

value <strong>of</strong> 77.<br />

On Conoids and Spheroids.<br />

The main problems attacked in this treatise are, in Archimedes's<br />

manner, stated in his preface addressed to Dositheus,<br />

which also sets out the premisses with regard to the solid<br />

figures in question.<br />

These premisses consist <strong>of</strong> definitions and<br />

obvious inferences from them. The figures are (1) the rightangled<br />

conoid (paraboloid <strong>of</strong> revolution), (2) the obtuse-angled<br />

conoid (hyperboloid <strong>of</strong> revolution), and (3) the spheroids<br />

(a) the oblong, described by the revolution <strong>of</strong> an ellipse about<br />

its 'greater diameter' (major axis), (b) the flat, described by<br />

the revolution <strong>of</strong> an ellipse about its lesser diameter ' ' (minor<br />

axis). Other definitions are those <strong>of</strong> the vertex and axis <strong>of</strong> the<br />

figures or segments there<strong>of</strong>, the vertex <strong>of</strong> a segment being<br />

the point <strong>of</strong> contact <strong>of</strong> the tangent plane to the solid which<br />

is parallel to the base <strong>of</strong> the segment. The centre is only<br />

recognized in the case <strong>of</strong> the spheroid ; what corresponds to<br />

the centre in the case <strong>of</strong> the hyperboloid is the ' vertex <strong>of</strong><br />

the enveloping cone ' (described by the revolution <strong>of</strong> what<br />

Archimedes calls the 'nearest lines to the section <strong>of</strong> the<br />

obtuse-angled cone', i.e. the asymptotes <strong>of</strong> the hyperbola),<br />

and the line between this point and the vertex <strong>of</strong> the hyperboloid<br />

or segment is<br />

called, not the axis or diameter, but (the<br />

line) 'adjacent to the axis'. The axis <strong>of</strong> the segment is in<br />

the case <strong>of</strong> the paraboloid the line through the vertex <strong>of</strong> the<br />

segment parallel to the axis <strong>of</strong> the paraboloid, in the case

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