An elementary treatment of the theory of spinning tops and gyroscopic motion, by Harold Crabtree.

OF THE INTRODUCTORY CHAPTER 49 But at the start w is very big, though it gradually diminishes under the action of the friction, and also the resistance of the air. Hence, at the start we have aw > AQ,..............................(i) i.e. the top is skidding and P is moving into the paper; friction accordingly acts in a direction which hurries the precession, and the top therefore rises. In the meantime w is diminishing (and also a as the top gets more vertical), and after a time we have ca = A,..............................(ii) i.e. P has no motion relative to the table, and steady rolling motion becomes possible. And, later, we have (a < A2,..............................(iii) i.e. friction is retarding" the precession and the top begins to fall. Were it not for the resistance of the air, the state of steady motion, when once established, would, theoretically, continue indefinitely: for as soon as aw becomes = A2 rolling commences, which can only be disturbed by air resistance. Immediately aw becomes < A2 friction acts so as to increase w, but never beyond the point necessary to maintain steady motion, since it is a self-adjusting force. Hence, the position of steady motion is a stable one, for friction produces an oscillating tendency to return to it; but eventually, the resistance of the air, tending to destroy this state, overcomes the tendency of friction to restore it. [13.] Even in vacuo the top would not really spin for ever. What is the explanation of this? [14.] In Fig. xvII. why must the gyroscope be placed on a smooth surface? [15.] The rougher the table the more quickly the top will rise when first spun. Why? [16.] Given a rough table, why does a top with a blunt peg rise more quickly than one with a fine peg? [17.] Explain the apparent contradiction of the tight and loose screw in the top of Figs. iv. (a) and iv. (b)..)l4. [18.] Supposing our object in spinning a top is to make it "go for as long as possible," how would (i) a blunt peg, (ii) a fine peg, contribute to length of time? [19.] How would the centre of gravity behave if the table were perfectly smooth? *It will be shown in Chapter IV. that, as the top dies, though friction is resisting precession, yet owing to other causes, Q increases. Amongst these is the fact that the gravity couple acts on a longer arm. D

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Title
An elementary treatment of the theory of spinning tops and gyroscopic motion, by Harold Crabtree.
Author
Crabtree, Harold.
Canvas
Page 47
Publication
London,: Longmans, Green, and co.,
1909.
Subject terms
Tops
Gyroscopes

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"An elementary treatment of the theory of spinning tops and gyroscopic motion, by Harold Crabtree." In the digital collection University of Michigan Historical Math Collection. https://name.umdl.umich.edu/abr4615.0001.001. University of Michigan Library Digital Collections. Accessed April 30, 2025.
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