An Elementary Treatise On the Theoretical Mechanics

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Fig. 70 CIRCULAR ARC 127 This relation shows tliat (the distance of c. G. Of arc 2 a from center) = cos — X (the distance of c. G. Of arc a from center). Similarly (the distance of c. G. Of arc a from center) = cos — X (the distance of c. G. Of arc — from center), and so on. Continuing in this "vvay, and substituting, we obtain (the distance of c. G. Of arc 2 a from center) a a a a = cos — ■ cos — • cos — . • . Cos 2 -i 8 2" + ^ X (the distance of c. G. Of arc — from center).
If we make n very
...great, the value of — becomes zero. Thus the dis- a " tance of the c. G. Of an arc — from the center becomes equal to a, the radius of the circle. JNIaking ?; infinite, we have (the distance of c. G. Of arc 2 a from center) = a cos — cos — cos — . • • to infinity. 2 4 8 -^ T, T a sin a ^ow cos — =, o a a ■ a 2 sin — o cos- = -' etc. , 4 1 • a ^ 4 sm — 4 a . 1, C( LL CC so that cos — • cos — • cos — 2 4 8 Makins: n infinite, the value of sin— becomes identical with -—, so a ' 2" 2 that 2" sin — becomes identical with a, and we have a a a j.

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