Scientific American Supplement, No. 362, December 9, 1882 by Various
page 22 of 140 (15%)
page 22 of 140 (15%)
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friction on the ring. This we accomplish by means of a shaft with whorls
on it, located directly over the drum for driving the spindle, from which bands drive each ring separately; and attached by cross-girts to the ring-rail, and moving up and down with it. This shaft is driven by a pair of conical drums from the main cylinder shaft, and is so arranged with a loose pulley on the large end of the receiving cone as to remain stationary while the wind is on or near the base of the bobbin, or nearly parallel to the path of the traveler. When the cone of the bobbin begins to diminish to such a point as to materially increase the radial pull on the traveler, these conical drums are put in operation by a belt shipper attached to the lift motion, which moves the belt on to the cones, and gives a continually accelerated motion to the rings, so that when the wind reaches the top of the bobbin the rings will have their maximum speed of about 300 revolutions per minute, or about one-twentieth the number of revolutions of the spindle at this point, if the latter make 6000 revolutions per minute, and this we find in actual practice to produce results which are highly satisfactory. As the lift falls again, the belt is moved back on the cones, giving a retarding motion to the rings, until it reaches the point at which it began to operate, and is then either moved on to the loose pulley, and the rings remain stationary, or for very fine yarn are kept in motion at a slow speed. We are often asked if this does not affect the twist, but answer that it does not in the least, as the relative speeds of the rolls and spindles remain the same, and the only thing that can be affected is the hardness of the wind upon the bobbin, and this is adjustable by the use of a heavier or lighter traveler, according to the |
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