MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System

Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Zhou, Xiaoming [verfasserIn] Huang, Hulin

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2009

Schlagwörter:	Magnetohydrodynamic(MHD) Thermocapillary convection Interface deformation VOF method

Anmerkung:	© Springer Science+Business Media B.V. 2009

Übergeordnetes Werk:	Enthalten in: Microgravity science and technology - Heidelberg : Springer, 2007, 22(2009), 2 vom: 17. Okt., Seite 185-191
Übergeordnetes Werk:	volume:22 ; year:2009 ; number:2 ; day:17 ; month:10 ; pages:185-191

Links:	Volltext

DOI / URN:	10.1007/s12217-009-9173-1

Katalog-ID:	SPR025394622

Internformat


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520			\|a Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface.
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650		4	\|a Thermocapillary convection \|7 (dpeaa)DE-He213
650		4	\|a Interface deformation \|7 (dpeaa)DE-He213
650		4	\|a VOF method \|7 (dpeaa)DE-He213
700	1		\|a Huang, Hulin \|4 aut
773	0	8	\|i Enthalten in \|t Microgravity science and technology \|d Heidelberg : Springer, 2007 \|g 22(2009), 2 vom: 17. Okt., Seite 185-191 \|w (DE-627)556726928 \|w (DE-600)2403671-7 \|x 1875-0494 \|7 nnns
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912			\|a GBV_ILN_65
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_150
912			\|a GBV_ILN_151
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_170
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_213
912			\|a GBV_ILN_224
912			\|a GBV_ILN_230
912			\|a GBV_ILN_250
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_636
912			\|a GBV_ILN_702
912			\|a GBV_ILN_2001
912			\|a GBV_ILN_2003
912			\|a GBV_ILN_2004
912			\|a GBV_ILN_2005
912			\|a GBV_ILN_2006
912			\|a GBV_ILN_2007
912			\|a GBV_ILN_2008
912			\|a GBV_ILN_2009
912			\|a GBV_ILN_2010
912			\|a GBV_ILN_2011
912			\|a GBV_ILN_2014
912			\|a GBV_ILN_2015
912			\|a GBV_ILN_2020
912			\|a GBV_ILN_2021
912			\|a GBV_ILN_2025
912			\|a GBV_ILN_2026
912			\|a GBV_ILN_2027
912			\|a GBV_ILN_2031
912			\|a GBV_ILN_2034
912			\|a GBV_ILN_2037
912			\|a GBV_ILN_2038
912			\|a GBV_ILN_2039
912			\|a GBV_ILN_2044
912			\|a GBV_ILN_2048
912			\|a GBV_ILN_2049
912			\|a GBV_ILN_2050
912			\|a GBV_ILN_2055
912			\|a GBV_ILN_2057
912			\|a GBV_ILN_2059
912			\|a GBV_ILN_2061
912			\|a GBV_ILN_2064
912			\|a GBV_ILN_2065
912			\|a GBV_ILN_2068
912			\|a GBV_ILN_2070
912			\|a GBV_ILN_2086
912			\|a GBV_ILN_2088
912			\|a GBV_ILN_2093
912			\|a GBV_ILN_2106
912			\|a GBV_ILN_2107
912			\|a GBV_ILN_2108
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912			\|a GBV_ILN_2116
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912			\|a GBV_ILN_2232
912			\|a GBV_ILN_2336
912			\|a GBV_ILN_2446
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912			\|a GBV_ILN_2472
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912			\|a GBV_ILN_2522
912			\|a GBV_ILN_2548
912			\|a GBV_ILN_4035
912			\|a GBV_ILN_4037
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912			\|a GBV_ILN_4333
912			\|a GBV_ILN_4334
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matchkey_str	article:18750494:2009----::hefcoitraileomtootemcplayovc
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publishDate	2009
allfields	10.1007/s12217-009-9173-1 doi (DE-627)SPR025394622 (SPR)s12217-009-9173-1-e DE-627 ger DE-627 rakwb eng Zhou, Xiaoming verfasserin aut MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. Magnetohydrodynamic(MHD) (dpeaa)DE-He213 Thermocapillary convection (dpeaa)DE-He213 Interface deformation (dpeaa)DE-He213 VOF method (dpeaa)DE-He213 Huang, Hulin aut Enthalten in Microgravity science and technology Heidelberg : Springer, 2007 22(2009), 2 vom: 17. Okt., Seite 185-191 (DE-627)556726928 (DE-600)2403671-7 1875-0494 nnns volume:22 year:2009 number:2 day:17 month:10 pages:185-191 https://dx.doi.org/10.1007/s12217-009-9173-1 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 22 2009 2 17 10 185-191
spelling	10.1007/s12217-009-9173-1 doi (DE-627)SPR025394622 (SPR)s12217-009-9173-1-e DE-627 ger DE-627 rakwb eng Zhou, Xiaoming verfasserin aut MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. Magnetohydrodynamic(MHD) (dpeaa)DE-He213 Thermocapillary convection (dpeaa)DE-He213 Interface deformation (dpeaa)DE-He213 VOF method (dpeaa)DE-He213 Huang, Hulin aut Enthalten in Microgravity science and technology Heidelberg : Springer, 2007 22(2009), 2 vom: 17. Okt., Seite 185-191 (DE-627)556726928 (DE-600)2403671-7 1875-0494 nnns volume:22 year:2009 number:2 day:17 month:10 pages:185-191 https://dx.doi.org/10.1007/s12217-009-9173-1 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 22 2009 2 17 10 185-191
allfields_unstemmed	10.1007/s12217-009-9173-1 doi (DE-627)SPR025394622 (SPR)s12217-009-9173-1-e DE-627 ger DE-627 rakwb eng Zhou, Xiaoming verfasserin aut MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. Magnetohydrodynamic(MHD) (dpeaa)DE-He213 Thermocapillary convection (dpeaa)DE-He213 Interface deformation (dpeaa)DE-He213 VOF method (dpeaa)DE-He213 Huang, Hulin aut Enthalten in Microgravity science and technology Heidelberg : Springer, 2007 22(2009), 2 vom: 17. Okt., Seite 185-191 (DE-627)556726928 (DE-600)2403671-7 1875-0494 nnns volume:22 year:2009 number:2 day:17 month:10 pages:185-191 https://dx.doi.org/10.1007/s12217-009-9173-1 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 22 2009 2 17 10 185-191
allfieldsGer	10.1007/s12217-009-9173-1 doi (DE-627)SPR025394622 (SPR)s12217-009-9173-1-e DE-627 ger DE-627 rakwb eng Zhou, Xiaoming verfasserin aut MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. Magnetohydrodynamic(MHD) (dpeaa)DE-He213 Thermocapillary convection (dpeaa)DE-He213 Interface deformation (dpeaa)DE-He213 VOF method (dpeaa)DE-He213 Huang, Hulin aut Enthalten in Microgravity science and technology Heidelberg : Springer, 2007 22(2009), 2 vom: 17. Okt., Seite 185-191 (DE-627)556726928 (DE-600)2403671-7 1875-0494 nnns volume:22 year:2009 number:2 day:17 month:10 pages:185-191 https://dx.doi.org/10.1007/s12217-009-9173-1 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 22 2009 2 17 10 185-191
allfieldsSound	10.1007/s12217-009-9173-1 doi (DE-627)SPR025394622 (SPR)s12217-009-9173-1-e DE-627 ger DE-627 rakwb eng Zhou, Xiaoming verfasserin aut MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System 2009 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier © Springer Science+Business Media B.V. 2009 Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. Magnetohydrodynamic(MHD) (dpeaa)DE-He213 Thermocapillary convection (dpeaa)DE-He213 Interface deformation (dpeaa)DE-He213 VOF method (dpeaa)DE-He213 Huang, Hulin aut Enthalten in Microgravity science and technology Heidelberg : Springer, 2007 22(2009), 2 vom: 17. Okt., Seite 185-191 (DE-627)556726928 (DE-600)2403671-7 1875-0494 nnns volume:22 year:2009 number:2 day:17 month:10 pages:185-191 https://dx.doi.org/10.1007/s12217-009-9173-1 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 22 2009 2 17 10 185-191
language	English
source	Enthalten in Microgravity science and technology 22(2009), 2 vom: 17. Okt., Seite 185-191 volume:22 year:2009 number:2 day:17 month:10 pages:185-191
sourceStr	Enthalten in Microgravity science and technology 22(2009), 2 vom: 17. Okt., Seite 185-191 volume:22 year:2009 number:2 day:17 month:10 pages:185-191
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Magnetohydrodynamic(MHD) Thermocapillary convection Interface deformation VOF method
isfreeaccess_bool	false
container_title	Microgravity science and technology
authorswithroles_txt_mv	Zhou, Xiaoming @@aut@@ Huang, Hulin @@aut@@
publishDateDaySort_date	2009-10-17T00:00:00Z
hierarchy_top_id	556726928
id	SPR025394622
language_de	englisch
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author	Zhou, Xiaoming
spellingShingle	Zhou, Xiaoming misc Magnetohydrodynamic(MHD) misc Thermocapillary convection misc Interface deformation misc VOF method MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System
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topic_title	MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System Magnetohydrodynamic(MHD) (dpeaa)DE-He213 Thermocapillary convection (dpeaa)DE-He213 Interface deformation (dpeaa)DE-He213 VOF method (dpeaa)DE-He213
topic	misc Magnetohydrodynamic(MHD) misc Thermocapillary convection misc Interface deformation misc VOF method
topic_unstemmed	misc Magnetohydrodynamic(MHD) misc Thermocapillary convection misc Interface deformation misc VOF method
topic_browse	misc Magnetohydrodynamic(MHD) misc Thermocapillary convection misc Interface deformation misc VOF method
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title	MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System
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title_full	MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System
author_sort	Zhou, Xiaoming
journal	Microgravity science and technology
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author_browse	Zhou, Xiaoming Huang, Hulin
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doi_str_mv	10.1007/s12217-009-9173-1
title_sort	mhd effect on interfacial deformation of thermocapillary convection in two-layer system
title_auth	MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System
abstract	Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. © Springer Science+Business Media B.V. 2009
abstractGer	Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. © Springer Science+Business Media B.V. 2009
abstract_unstemmed	Abstract Effect of magnetic field on interfacial deformation of thermocapillary convection in a two-layer fluid system under microgravity condition is investigated. The upper layer fluid is silicon oil, the lower layer fluid is InBi. The dynamic conditions at free surface are implemented through the continuum surface force (CSF) model with the volume of fluid (VOF) method. The induction magnetic field method is used. The results show that, the interface bulges out at the hot end and bulges in at the cold end without magnetohydrodynamic (MHD) and the interface deformation is dominated by dynamic pressure. Under the influence of magnetic field, the interface deformability decreases with increasing of Hartmann number, and the interface deformation can be fully suppressed while the Hartmann number is enough large and the damping of magnetic field on the deformation of interface mainly concentrated at the region close to the interface. © Springer Science+Business Media B.V. 2009
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title_short	MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System
url	https://dx.doi.org/10.1007/s12217-009-9173-1
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up_date	2024-07-03T15:44:32.764Z
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MHD Effect on Interfacial Deformation of Thermocapillary Convection in Two-Layer System

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