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The theory of compacting
By :   Peter Stahlecker
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Now, imagine a fibre B coming out of the front nipping point at a distance d from fibre A. It suffers the same fate so to speak. It will also be unable to cross the downstream edge of the slot and will align itself closely to fibre A, as they move to the end of the slot.


Thus, a fibre bundle having a certain width upon leaving the front nipping point, and with the individual fibres neither parallel nor stretched, is transformed into a bundle where the fibres are perfectly parallel and close to each other.


Naturally, the two effects complement each other, but it is obvious that the second effect is several orders of magnitude larger than the first one; also only the second effect stretches the fibres at the same time. As may be imagined, there is a complicated relationship between the optimum angle α, the suction pressure and the properties of the various fibres.


If the compacting system allows V0, the speed of the perforated means to be varied relative to the speed of the front roller, the stretching of the fibres may be controlled further.


Much of these important details are not yet understood well theoretically, and as so often in spinning one must rely on experience, and one finds surprises every once in a while!


About the Author:


The author is the Managing Director of Spindelfabrik Suessen GmbH.


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Published On Thursday, July 17, 2008
 
 
 

 
 
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