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DC Field | Value | Language |
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dc.contributor.author | Das, Ramyaranjan | - |
dc.contributor.author | Ranjan, Mukesh | - |
dc.contributor.author | Bisoyi, Dillip Kumar | - |
dc.date.accessioned | 2024-11-27T04:54:23Z | - |
dc.date.available | 2024-11-27T04:54:23Z | - |
dc.date.issued | 2024-11 | - |
dc.identifier.citation | 19th International Small-Angle Scattering Conference (SAS), TICC, Taipei, Taiwan, 03-08 November 2024 | en_US |
dc.identifier.uri | http://hdl.handle.net/2080/4772 | - |
dc.description | Copyright belongs to proceeding publisher | en_US |
dc.description.abstract | The macromolecular structure of untreated and cold plasma-treated cellulosic kapok fiber was investigated by means of small-angle X-ray scattering (SAXS) and wide-angle X-ray diffraction (WAXD). Subsequently, the macromolecular structural transition of the fiber was correlated with the dielectric properties of their reinforced epoxy polymer composites. WAXD patterns of the fibers resemble the cellulose Iπ½ structure of the cellulose. The X-ray diffractogram of untreated and treated fiber samples shows typical cellulose Iπ½ peaks within the Bragg Diffraction angle 10Β° to 50Β° (2πο» 16.68Β° (1-10/110), 22.42Β° (200) and 34.82Β° (004)). The crystallinity index (CI) and crystallite size (CS) are calculated using Segals and Scherrerβs formula respectively. The one-dimensional and three-dimensional correlation functions are calculated from background-corrected smeared-out SAXS intensities [1]. The SAXS profile of the fiber showed drastic change, with cold plasma treatment and the intensities at the tail region deviate from the porodβs law which conforms the non-ideal nature of the fiber, signifying the continuous variation of electron density at the phase boundary [2,3]. Further, the theories developed by Vonk and Ruland were used to estimate different macromolecular parameters such as transversal length in the matter region (π1Μ ), transversal length in the void region (π2Μ ), periodicity transverse to the layers (π·), the width of the transition layer (πΈ) by Ruland and Vonk method, specific inner surface area (π /π£), matter phase volume fraction (Ο1), void phase volume fraction (Ο2), the volume fraction of transition layer (2πΈππ·) coherence length (ππΆ), range of inhomogeneity (ππΜ ) and characteristic number (ππΆ) from correlation functions, considering the fiber has a non-ideal two-phase structure [1-3]. A Fortran program developed by our research group is used to investigate the SAXS data and calculate different macromolecular parameters. | en_US |
dc.subject | Small-angle X-ray scattering (SAXS) | en_US |
dc.subject | Macromolecular structure | en_US |
dc.subject | Cold plasma | en_US |
dc.subject | Polymer composites | en_US |
dc.title | The Macromolecular Transition of Kapok Fiber by Cold Plasma Treatment as Investigated by SAXS/WAXD Studies and Their Correlation with Electrical Properties of the Fiber-Reinforced Composites | en_US |
dc.type | Presentation | en_US |
Appears in Collections: | Conference Papers |
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2024_SAS_RDas_Macromolecular.pdf | Poster | 2.47 MB | Adobe PDF | View/Open Request a copy |
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