Three-dimensional numerical simulation of the movement of the flexible body under different constraints
Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Jin, Yuzhen [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: |
© Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of thermal science - Berlin : Springer, 1992, 23(2014), 6 vom: 22. Nov., Seite 593-599 |
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| Übergeordnetes Werk: |
volume:23 ; year:2014 ; number:6 ; day:22 ; month:11 ; pages:593-599 |
| Links: |
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| DOI / URN: |
10.1007/s11630-014-0746-y |
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| Katalog-ID: |
SPR02126614X |
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| 100 | 1 | |a Jin, Yuzhen |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Three-dimensional numerical simulation of the movement of the flexible body under different constraints |
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| 520 | |a Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. | ||
| 650 | 4 | |a fluid-structure interaction |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a numerical simulation |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a flexible body |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a adaptive grid control method |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Li, Jun |4 aut | |
| 700 | 1 | |a Zhu, Linhang |4 aut | |
| 700 | 1 | |a Du, Jiayou |4 aut | |
| 700 | 1 | |a Jin, Yingzi |4 aut | |
| 700 | 1 | |a Lin, Peifeng |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Journal of thermal science |d Berlin : Springer, 1992 |g 23(2014), 6 vom: 22. Nov., Seite 593-599 |w (DE-627)528360884 |w (DE-600)2280144-3 |x 1993-033X |7 nnns |
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10.1007/s11630-014-0746-y doi (DE-627)SPR02126614X (SPR)s11630-014-0746-y-e DE-627 ger DE-627 rakwb eng Jin, Yuzhen verfasserin aut Three-dimensional numerical simulation of the movement of the flexible body under different constraints 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. fluid-structure interaction (dpeaa)DE-He213 numerical simulation (dpeaa)DE-He213 flexible body (dpeaa)DE-He213 adaptive grid control method (dpeaa)DE-He213 Li, Jun aut Zhu, Linhang aut Du, Jiayou aut Jin, Yingzi aut Lin, Peifeng aut Enthalten in Journal of thermal science Berlin : Springer, 1992 23(2014), 6 vom: 22. Nov., Seite 593-599 (DE-627)528360884 (DE-600)2280144-3 1993-033X nnns volume:23 year:2014 number:6 day:22 month:11 pages:593-599 https://dx.doi.org/10.1007/s11630-014-0746-y 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_101 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 23 2014 6 22 11 593-599 |
| spelling |
10.1007/s11630-014-0746-y doi (DE-627)SPR02126614X (SPR)s11630-014-0746-y-e DE-627 ger DE-627 rakwb eng Jin, Yuzhen verfasserin aut Three-dimensional numerical simulation of the movement of the flexible body under different constraints 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. fluid-structure interaction (dpeaa)DE-He213 numerical simulation (dpeaa)DE-He213 flexible body (dpeaa)DE-He213 adaptive grid control method (dpeaa)DE-He213 Li, Jun aut Zhu, Linhang aut Du, Jiayou aut Jin, Yingzi aut Lin, Peifeng aut Enthalten in Journal of thermal science Berlin : Springer, 1992 23(2014), 6 vom: 22. Nov., Seite 593-599 (DE-627)528360884 (DE-600)2280144-3 1993-033X nnns volume:23 year:2014 number:6 day:22 month:11 pages:593-599 https://dx.doi.org/10.1007/s11630-014-0746-y 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_101 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 23 2014 6 22 11 593-599 |
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10.1007/s11630-014-0746-y doi (DE-627)SPR02126614X (SPR)s11630-014-0746-y-e DE-627 ger DE-627 rakwb eng Jin, Yuzhen verfasserin aut Three-dimensional numerical simulation of the movement of the flexible body under different constraints 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. fluid-structure interaction (dpeaa)DE-He213 numerical simulation (dpeaa)DE-He213 flexible body (dpeaa)DE-He213 adaptive grid control method (dpeaa)DE-He213 Li, Jun aut Zhu, Linhang aut Du, Jiayou aut Jin, Yingzi aut Lin, Peifeng aut Enthalten in Journal of thermal science Berlin : Springer, 1992 23(2014), 6 vom: 22. Nov., Seite 593-599 (DE-627)528360884 (DE-600)2280144-3 1993-033X nnns volume:23 year:2014 number:6 day:22 month:11 pages:593-599 https://dx.doi.org/10.1007/s11630-014-0746-y 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_101 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 23 2014 6 22 11 593-599 |
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10.1007/s11630-014-0746-y doi (DE-627)SPR02126614X (SPR)s11630-014-0746-y-e DE-627 ger DE-627 rakwb eng Jin, Yuzhen verfasserin aut Three-dimensional numerical simulation of the movement of the flexible body under different constraints 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. fluid-structure interaction (dpeaa)DE-He213 numerical simulation (dpeaa)DE-He213 flexible body (dpeaa)DE-He213 adaptive grid control method (dpeaa)DE-He213 Li, Jun aut Zhu, Linhang aut Du, Jiayou aut Jin, Yingzi aut Lin, Peifeng aut Enthalten in Journal of thermal science Berlin : Springer, 1992 23(2014), 6 vom: 22. Nov., Seite 593-599 (DE-627)528360884 (DE-600)2280144-3 1993-033X nnns volume:23 year:2014 number:6 day:22 month:11 pages:593-599 https://dx.doi.org/10.1007/s11630-014-0746-y 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_101 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 23 2014 6 22 11 593-599 |
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10.1007/s11630-014-0746-y doi (DE-627)SPR02126614X (SPR)s11630-014-0746-y-e DE-627 ger DE-627 rakwb eng Jin, Yuzhen verfasserin aut Three-dimensional numerical simulation of the movement of the flexible body under different constraints 2014 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. fluid-structure interaction (dpeaa)DE-He213 numerical simulation (dpeaa)DE-He213 flexible body (dpeaa)DE-He213 adaptive grid control method (dpeaa)DE-He213 Li, Jun aut Zhu, Linhang aut Du, Jiayou aut Jin, Yingzi aut Lin, Peifeng aut Enthalten in Journal of thermal science Berlin : Springer, 1992 23(2014), 6 vom: 22. Nov., Seite 593-599 (DE-627)528360884 (DE-600)2280144-3 1993-033X nnns volume:23 year:2014 number:6 day:22 month:11 pages:593-599 https://dx.doi.org/10.1007/s11630-014-0746-y 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_101 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_4012 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 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 23 2014 6 22 11 593-599 |
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Enthalten in Journal of thermal science 23(2014), 6 vom: 22. Nov., Seite 593-599 volume:23 year:2014 number:6 day:22 month:11 pages:593-599 |
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Enthalten in Journal of thermal science 23(2014), 6 vom: 22. Nov., Seite 593-599 volume:23 year:2014 number:6 day:22 month:11 pages:593-599 |
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Jin, Yuzhen @@aut@@ Li, Jun @@aut@@ Zhu, Linhang @@aut@@ Du, Jiayou @@aut@@ Jin, Yingzi @@aut@@ Lin, Peifeng @@aut@@ |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR02126614X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331075336.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2014 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11630-014-0746-y</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR02126614X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s11630-014-0746-y-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Jin, Yuzhen</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Three-dimensional numerical simulation of the movement of the flexible body under different constraints</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2014</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">fluid-structure interaction</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">numerical simulation</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">flexible body</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">adaptive grid control method</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Li, Jun</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zhu, Linhang</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Du, Jiayou</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Jin, Yingzi</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Lin, Peifeng</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of thermal science</subfield><subfield code="d">Berlin : Springer, 1992</subfield><subfield code="g">23(2014), 6 vom: 22. 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Jin, Yuzhen |
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Jin, Yuzhen misc fluid-structure interaction misc numerical simulation misc flexible body misc adaptive grid control method Three-dimensional numerical simulation of the movement of the flexible body under different constraints |
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Three-dimensional numerical simulation of the movement of the flexible body under different constraints fluid-structure interaction (dpeaa)DE-He213 numerical simulation (dpeaa)DE-He213 flexible body (dpeaa)DE-He213 adaptive grid control method (dpeaa)DE-He213 |
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Jin, Yuzhen Li, Jun Zhu, Linhang Du, Jiayou Jin, Yingzi Lin, Peifeng |
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three-dimensional numerical simulation of the movement of the flexible body under different constraints |
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Three-dimensional numerical simulation of the movement of the flexible body under different constraints |
| abstract |
Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 |
| abstractGer |
Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 |
| abstract_unstemmed |
Abstract For the large deformation of the flexible body may cause the fluid grid distortion, which will make the numerical calculation tedious, even to end, the numerical simulation of the flexible body coupling with the fluid is always a tough problem. In this paper, the flexible body is under two kinds of constrained conditions and the ratio of length-diameter is 1:30. The Reynolds number of the airflow is 513, belonging to the area of low Reynolds number. The control equations of the coupling of flexible body with airflow are built and the adaptive grid control method is adopted to conduct the three-dimensional numerical simulation of the movement of the flexible body. The numerical results show that it is possible to simulate the characteristics of the flexible body’s movement in the low Reynolds number airflow when the appropriate control equations are modeled and suitable equation-solving method is adopted. Unconstrained flexible body would turn over forward along the airflow’s diffusion direction, while constrained flexible body in the flow field will make periodic rotation motion along the axis of the flexible body, and the bending deformation is more obvious than that of unconstrained flexible body. The preliminary three-dimensional numerical simulation can provide references for further research on the characteristics of the yarn movement in high Reynolds number airflow. © Science Press, Institute of Engineering Thermophysics, CAS and Springer-Verlag Berlin Heidelberg 2014 |
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Three-dimensional numerical simulation of the movement of the flexible body under different constraints |
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| author2 |
Li, Jun Zhu, Linhang Du, Jiayou Jin, Yingzi Lin, Peifeng |
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Li, Jun Zhu, Linhang Du, Jiayou Jin, Yingzi Lin, Peifeng |
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10.1007/s11630-014-0746-y |
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| score |
7.4019136 |