Applied Mechanics for Engineers; a Text-Book for Engineering Students

Cover Applied Mechanics for Engineers; a Text-Book for Engineering Students
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It follows that t)^ = — r sin ^ -^ = — >'a> sin ; _ k d^_a)k -^ is the angular velocity of the point with respect to 2; I F represent it by a (see Art. 95), so that v = -^ = —ra> cos ; a„ = r sin A-^ = — ra> sin .
That is, the acceleration in the direction of the resultant force is equal to cor and the accelerating force is equal to Mior.
The fact of zero tangential accelerations has made this curve very useful. In many cases the helical surface formed by the revolving line has been made use o
...f to send packages from upper floors of commercial establish- ments to the lower floors. Since a^ = 0, the packages move down with uniform motion. The helicoid is in- closed in a tube with convenient openings for the insertion of packages.

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