Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct
Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for t...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Lin, Jian-zhong [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2014 |
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| Schlagwörter: |
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| Anmerkung: |
© The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 |
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| Übergeordnetes Werk: |
Enthalten in: Fibers and polymers - Seoul : The Korean Fiber Society, 2000, 15(2014), 2 vom: Feb., Seite 364-372 |
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| Übergeordnetes Werk: |
volume:15 ; year:2014 ; number:2 ; month:02 ; pages:364-372 |
| Links: |
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| DOI / URN: |
10.1007/s12221-014-0364-z |
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| Katalog-ID: |
SPR025428160 |
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| 245 | 1 | 0 | |a Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct |
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| 520 | |a Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. | ||
| 650 | 4 | |a Fiber suspension |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Fiber orientation |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Curved expansion duct |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Rotating |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Zhang, Qi-hua |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Fibers and polymers |d Seoul : The Korean Fiber Society, 2000 |g 15(2014), 2 vom: Feb., Seite 364-372 |w (DE-627)565516485 |w (DE-600)2424081-3 |x 1875-0052 |7 nnns |
| 773 | 1 | 8 | |g volume:15 |g year:2014 |g number:2 |g month:02 |g pages:364-372 |
| 856 | 4 | 0 | |u https://dx.doi.org/10.1007/s12221-014-0364-z |z lizenzpflichtig |3 Volltext |
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10.1007/s12221-014-0364-z doi (DE-627)SPR025428160 (SPR)s12221-014-0364-z-e DE-627 ger DE-627 rakwb eng Lin, Jian-zhong verfasserin aut Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. Fiber suspension (dpeaa)DE-He213 Fiber orientation (dpeaa)DE-He213 Curved expansion duct (dpeaa)DE-He213 Rotating (dpeaa)DE-He213 Zhang, Qi-hua aut Enthalten in Fibers and polymers Seoul : The Korean Fiber Society, 2000 15(2014), 2 vom: Feb., Seite 364-372 (DE-627)565516485 (DE-600)2424081-3 1875-0052 nnns volume:15 year:2014 number:2 month:02 pages:364-372 https://dx.doi.org/10.1007/s12221-014-0364-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 2 02 364-372 |
| spelling |
10.1007/s12221-014-0364-z doi (DE-627)SPR025428160 (SPR)s12221-014-0364-z-e DE-627 ger DE-627 rakwb eng Lin, Jian-zhong verfasserin aut Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. Fiber suspension (dpeaa)DE-He213 Fiber orientation (dpeaa)DE-He213 Curved expansion duct (dpeaa)DE-He213 Rotating (dpeaa)DE-He213 Zhang, Qi-hua aut Enthalten in Fibers and polymers Seoul : The Korean Fiber Society, 2000 15(2014), 2 vom: Feb., Seite 364-372 (DE-627)565516485 (DE-600)2424081-3 1875-0052 nnns volume:15 year:2014 number:2 month:02 pages:364-372 https://dx.doi.org/10.1007/s12221-014-0364-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 2 02 364-372 |
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10.1007/s12221-014-0364-z doi (DE-627)SPR025428160 (SPR)s12221-014-0364-z-e DE-627 ger DE-627 rakwb eng Lin, Jian-zhong verfasserin aut Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. Fiber suspension (dpeaa)DE-He213 Fiber orientation (dpeaa)DE-He213 Curved expansion duct (dpeaa)DE-He213 Rotating (dpeaa)DE-He213 Zhang, Qi-hua aut Enthalten in Fibers and polymers Seoul : The Korean Fiber Society, 2000 15(2014), 2 vom: Feb., Seite 364-372 (DE-627)565516485 (DE-600)2424081-3 1875-0052 nnns volume:15 year:2014 number:2 month:02 pages:364-372 https://dx.doi.org/10.1007/s12221-014-0364-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 2 02 364-372 |
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10.1007/s12221-014-0364-z doi (DE-627)SPR025428160 (SPR)s12221-014-0364-z-e DE-627 ger DE-627 rakwb eng Lin, Jian-zhong verfasserin aut Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. Fiber suspension (dpeaa)DE-He213 Fiber orientation (dpeaa)DE-He213 Curved expansion duct (dpeaa)DE-He213 Rotating (dpeaa)DE-He213 Zhang, Qi-hua aut Enthalten in Fibers and polymers Seoul : The Korean Fiber Society, 2000 15(2014), 2 vom: Feb., Seite 364-372 (DE-627)565516485 (DE-600)2424081-3 1875-0052 nnns volume:15 year:2014 number:2 month:02 pages:364-372 https://dx.doi.org/10.1007/s12221-014-0364-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 2 02 364-372 |
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10.1007/s12221-014-0364-z doi (DE-627)SPR025428160 (SPR)s12221-014-0364-z-e DE-627 ger DE-627 rakwb eng Lin, Jian-zhong verfasserin aut Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. Fiber suspension (dpeaa)DE-He213 Fiber orientation (dpeaa)DE-He213 Curved expansion duct (dpeaa)DE-He213 Rotating (dpeaa)DE-He213 Zhang, Qi-hua aut Enthalten in Fibers and polymers Seoul : The Korean Fiber Society, 2000 15(2014), 2 vom: Feb., Seite 364-372 (DE-627)565516485 (DE-600)2424081-3 1875-0052 nnns volume:15 year:2014 number:2 month:02 pages:364-372 https://dx.doi.org/10.1007/s12221-014-0364-z lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_65 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2008 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 AR 15 2014 2 02 364-372 |
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Enthalten in Fibers and polymers 15(2014), 2 vom: Feb., Seite 364-372 volume:15 year:2014 number:2 month:02 pages:364-372 |
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Enthalten in Fibers and polymers 15(2014), 2 vom: Feb., Seite 364-372 volume:15 year:2014 number:2 month:02 pages:364-372 |
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Lin, Jian-zhong @@aut@@ Zhang, Qi-hua @@aut@@ |
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Lin, Jian-zhong |
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Lin, Jian-zhong misc Fiber suspension misc Fiber orientation misc Curved expansion duct misc Rotating Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct |
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Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct Fiber suspension (dpeaa)DE-He213 Fiber orientation (dpeaa)DE-He213 Curved expansion duct (dpeaa)DE-He213 Rotating (dpeaa)DE-He213 |
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misc Fiber suspension misc Fiber orientation misc Curved expansion duct misc Rotating |
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misc Fiber suspension misc Fiber orientation misc Curved expansion duct misc Rotating |
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Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct |
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Lin, Jian-zhong |
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three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct |
| title_auth |
Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct |
| abstract |
Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 |
| abstractGer |
Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 |
| abstract_unstemmed |
Abstract A complete three-dimensional Jeffery equation is solved through both analytical and numerical method to obtain the orientation evolution of a single fiber rotating in a shear flow. The orientation evolutions of a single fiber under different conditions are given. A more complete model for the simulation of fiber orientation is presented and combined with the Runge-Kutta algorithm to obtain the evolution of fiber orientation in the fiber suspensions through a rotating curved expansion duct. The numerical results show that the evolution of fiber orientation along the duct in different cross-sections is quite different. The fiber orientations change drastically in the vicinity of the inlet and then change slowly along the flow direction. The inlet velocity has little effect on the evolution of fiber orientation, but a great effect on the trajectory of the fiber. The effect of the initial fiber orientation on the evolution of fiber orientation is contrary to that of inlet velocity. The effect of rotation rate on the evolution of fiber orientation is much smaller than that of inlet velocity. Near the concave wall region the smaller the fiber aspect ratio is, the more drastically the fibers swing. The fibers near the centerline and the convex wall region do not show a swing. Studying such complex flow will beneficially contribute to reach a better understanding of flow properties in many important manufacturing processes to make composites. © The Korean Fiber Society and Springer Science+Business Media Dordrecht 2014 |
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Three-dimensional fiber orientation of fiber suspensions flowing through a rotating curved expansion duct |
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https://dx.doi.org/10.1007/s12221-014-0364-z |
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Zhang, Qi-hua |
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10.1007/s12221-014-0364-z |
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