Please use this identifier to cite or link to this item: http://nopr.niscpr.res.in/handle/123456789/24709
Full metadata record
DC FieldValueLanguage
dc.contributor.authorNeckar, Bohuslav-
dc.contributor.authorDas, Dipayan-
dc.date.accessioned2013-12-12T06:38:22Z-
dc.date.available2013-12-12T06:38:22Z-
dc.date.issued2005-12-
dc.identifier.issn0975-1025 (Online); 0971-0426 (Print)-
dc.identifier.urihttp://hdl.handle.net/123456789/24709-
dc.description421-430en_US
dc.description.abstractA new method has been reported for the evaluation of yarn unevenness spectrogram of the Uster Tester 3. The process to establish the theoretical relation between the spectral analysis and the autocorrelation function of yarn unevenness is demonstrated with the help of a practical example. It is observed that the random process of mass variation along a yarn is more expressible as an infinite sum of harmonic functions (integral) having infinitesimal amplitudes as compared to when the random process is expressed simply as a sum of harmonic functions. en_US
dc.language.isoen_USen_US
dc.publisherNISCAIR-CSIR, Indiaen_US
dc.relation.ispartofseriesInt.CI.7 D02G3/00en_US
dc.rights CC Attribution-Noncommercial-No Derivative Works 2.5 Indiaen_US
dc.sourceIJFTR Vol.30(4) [December 2005]en_US
dc.subjectAutocorrelation functionen_US
dc.subjectSpectral density functionen_US
dc.subjectYarn unevennessen_US
dc.titleAutocorrelation function of yarn unevennessen_US
dc.typeArticleen_US
Appears in Collections:IJFTR Vol.30(4) [December 2005]

Files in This Item:
File Description SizeFormat 
IJFTR 30(4) 421-430.pdf4.02 MBAdobe PDFView/Open


Items in NOPR are protected by copyright, with all rights reserved, unless otherwise indicated.