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A history of Greek mathematics - Wilbourhall.org

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76 ARCHIMEDES<br />

pro<strong>of</strong>s.<br />

We do not find him here assuming, as in The Method,<br />

that, if all the lines that can be drawn in a figure parallel<br />

(and including) one side have their middle points in a straight<br />

line, the centre <strong>of</strong> gravity must lie somewhere on that straight<br />

line ; he is not content to regard the figure as made up <strong>of</strong> an<br />

infinity <strong>of</strong> such parallel lines ;<br />

pure geometry realizes that<br />

the parallelogram is made up <strong>of</strong> elementary parallelograms,<br />

indefinitely narrow if you please, but still parallelograms, and<br />

the triangle <strong>of</strong> elementary trapezia, not straight lines, so<br />

that to assume directly that the centre <strong>of</strong> gravity lies on the<br />

straight line bisecting the parallelograms would really be<br />

a i^etitio principii. Accordingly the result, no doubt discovered<br />

in the informal way, is clinched by a pro<strong>of</strong> by reductio<br />

ad absardum in each case. In the case <strong>of</strong> the parallelogram<br />

ABCD (Prop. 9), if the centre <strong>of</strong> gravity is not on the straight<br />

line EF bisecting two opposite sides, let it be at H. Draw<br />

HK parallel to AD. Then it is possible by bisecting AE, ED,<br />

then bisecting the halves, and so on, ultimately to reach<br />

a length less than KH. Let this be done, and through the<br />

to<br />

points <strong>of</strong> division <strong>of</strong> AD draw parallels to AB or DC making<br />

a number <strong>of</strong> equal and similar parallelograms as in the figure.<br />

The centre <strong>of</strong> gravity <strong>of</strong> each <strong>of</strong> these parallelograms is<br />

similarly situated with regard to it.<br />

Hence we have a number<br />

<strong>of</strong> equal magnitudes with their centres <strong>of</strong> gravity at equal<br />

distances along a straight line. Therefore the centre <strong>of</strong><br />

gravity <strong>of</strong> the whole is on the line joining the centres <strong>of</strong> gravity<br />

<strong>of</strong> the two middle parallelograms (Prop. 5, Cor. 2). But this<br />

is impossible, because H is outside those parallelograms.<br />

Therefore the centre <strong>of</strong> gravity cannot but lie on EF.<br />

Similarly the centre <strong>of</strong> gravity lies on the straight line<br />

bisecting the other opposite sides AB, CD; therefore it lies at<br />

the intersection <strong>of</strong> this line with EF, i.e. at the point <strong>of</strong><br />

intersection <strong>of</strong> the diagonals.

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