The movement and shape change characteristics of a bubble passing through a liquid-liquid interface
In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results...
Ausführliche Beschreibung
Autor*in: |
Xu Jiarui [verfasserIn] Zhang Xiaohui [verfasserIn] Qing Shan [verfasserIn] Wu Jiaying [verfasserIn] |
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Format: |
E-Artikel |
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Sprache: |
Englisch |
Erschienen: |
2023 |
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Übergeordnetes Werk: |
In: Thermal Science - VINCA Institute of Nuclear Sciences, 2006, 27(2023), 1 Part A, Seite 207-217 |
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Übergeordnetes Werk: |
volume:27 ; year:2023 ; number:1 Part A ; pages:207-217 |
Links: |
Link aufrufen |
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DOI / URN: |
10.2298/TSCI220307123X |
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Katalog-ID: |
DOAJ088051625 |
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520 | |a In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. | ||
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10.2298/TSCI220307123X doi (DE-627)DOAJ088051625 (DE-599)DOAJ5f3916ea63b749d5bd438686c7c771df DE-627 ger DE-627 rakwb eng TJ1-1570 Xu Jiarui verfasserin aut The movement and shape change characteristics of a bubble passing through a liquid-liquid interface 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. multiphase flow single bubble shape analysis immiscible fluids rising behavior Mechanical engineering and machinery Zhang Xiaohui verfasserin aut Qing Shan verfasserin aut Wu Jiaying verfasserin aut In Thermal Science VINCA Institute of Nuclear Sciences, 2006 27(2023), 1 Part A, Seite 207-217 (DE-627)514240016 (DE-600)2241319-4 23347163 nnns volume:27 year:2023 number:1 Part A pages:207-217 https://doi.org/10.2298/TSCI220307123X kostenfrei https://doaj.org/article/5f3916ea63b749d5bd438686c7c771df kostenfrei http://www.doiserbia.nb.rs/img/doi/0354-9836/2023/0354-98362200123X.pdf kostenfrei https://doaj.org/toc/0354-9836 Journal toc kostenfrei https://doaj.org/toc/2334-7163 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 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_2031 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 27 2023 1 Part A 207-217 |
spelling |
10.2298/TSCI220307123X doi (DE-627)DOAJ088051625 (DE-599)DOAJ5f3916ea63b749d5bd438686c7c771df DE-627 ger DE-627 rakwb eng TJ1-1570 Xu Jiarui verfasserin aut The movement and shape change characteristics of a bubble passing through a liquid-liquid interface 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. multiphase flow single bubble shape analysis immiscible fluids rising behavior Mechanical engineering and machinery Zhang Xiaohui verfasserin aut Qing Shan verfasserin aut Wu Jiaying verfasserin aut In Thermal Science VINCA Institute of Nuclear Sciences, 2006 27(2023), 1 Part A, Seite 207-217 (DE-627)514240016 (DE-600)2241319-4 23347163 nnns volume:27 year:2023 number:1 Part A pages:207-217 https://doi.org/10.2298/TSCI220307123X kostenfrei https://doaj.org/article/5f3916ea63b749d5bd438686c7c771df kostenfrei http://www.doiserbia.nb.rs/img/doi/0354-9836/2023/0354-98362200123X.pdf kostenfrei https://doaj.org/toc/0354-9836 Journal toc kostenfrei https://doaj.org/toc/2334-7163 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 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_2031 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 27 2023 1 Part A 207-217 |
allfields_unstemmed |
10.2298/TSCI220307123X doi (DE-627)DOAJ088051625 (DE-599)DOAJ5f3916ea63b749d5bd438686c7c771df DE-627 ger DE-627 rakwb eng TJ1-1570 Xu Jiarui verfasserin aut The movement and shape change characteristics of a bubble passing through a liquid-liquid interface 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. multiphase flow single bubble shape analysis immiscible fluids rising behavior Mechanical engineering and machinery Zhang Xiaohui verfasserin aut Qing Shan verfasserin aut Wu Jiaying verfasserin aut In Thermal Science VINCA Institute of Nuclear Sciences, 2006 27(2023), 1 Part A, Seite 207-217 (DE-627)514240016 (DE-600)2241319-4 23347163 nnns volume:27 year:2023 number:1 Part A pages:207-217 https://doi.org/10.2298/TSCI220307123X kostenfrei https://doaj.org/article/5f3916ea63b749d5bd438686c7c771df kostenfrei http://www.doiserbia.nb.rs/img/doi/0354-9836/2023/0354-98362200123X.pdf kostenfrei https://doaj.org/toc/0354-9836 Journal toc kostenfrei https://doaj.org/toc/2334-7163 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 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_2031 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 27 2023 1 Part A 207-217 |
allfieldsGer |
10.2298/TSCI220307123X doi (DE-627)DOAJ088051625 (DE-599)DOAJ5f3916ea63b749d5bd438686c7c771df DE-627 ger DE-627 rakwb eng TJ1-1570 Xu Jiarui verfasserin aut The movement and shape change characteristics of a bubble passing through a liquid-liquid interface 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. multiphase flow single bubble shape analysis immiscible fluids rising behavior Mechanical engineering and machinery Zhang Xiaohui verfasserin aut Qing Shan verfasserin aut Wu Jiaying verfasserin aut In Thermal Science VINCA Institute of Nuclear Sciences, 2006 27(2023), 1 Part A, Seite 207-217 (DE-627)514240016 (DE-600)2241319-4 23347163 nnns volume:27 year:2023 number:1 Part A pages:207-217 https://doi.org/10.2298/TSCI220307123X kostenfrei https://doaj.org/article/5f3916ea63b749d5bd438686c7c771df kostenfrei http://www.doiserbia.nb.rs/img/doi/0354-9836/2023/0354-98362200123X.pdf kostenfrei https://doaj.org/toc/0354-9836 Journal toc kostenfrei https://doaj.org/toc/2334-7163 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 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_2031 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 27 2023 1 Part A 207-217 |
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10.2298/TSCI220307123X doi (DE-627)DOAJ088051625 (DE-599)DOAJ5f3916ea63b749d5bd438686c7c771df DE-627 ger DE-627 rakwb eng TJ1-1570 Xu Jiarui verfasserin aut The movement and shape change characteristics of a bubble passing through a liquid-liquid interface 2023 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. multiphase flow single bubble shape analysis immiscible fluids rising behavior Mechanical engineering and machinery Zhang Xiaohui verfasserin aut Qing Shan verfasserin aut Wu Jiaying verfasserin aut In Thermal Science VINCA Institute of Nuclear Sciences, 2006 27(2023), 1 Part A, Seite 207-217 (DE-627)514240016 (DE-600)2241319-4 23347163 nnns volume:27 year:2023 number:1 Part A pages:207-217 https://doi.org/10.2298/TSCI220307123X kostenfrei https://doaj.org/article/5f3916ea63b749d5bd438686c7c771df kostenfrei http://www.doiserbia.nb.rs/img/doi/0354-9836/2023/0354-98362200123X.pdf kostenfrei https://doaj.org/toc/0354-9836 Journal toc kostenfrei https://doaj.org/toc/2334-7163 Journal toc kostenfrei GBV_USEFLAG_A SYSFLAG_A GBV_DOAJ SSG-OLC-PHA GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 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_95 GBV_ILN_105 GBV_ILN_110 GBV_ILN_151 GBV_ILN_161 GBV_ILN_170 GBV_ILN_206 GBV_ILN_213 GBV_ILN_230 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2005 GBV_ILN_2006 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_2031 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2056 GBV_ILN_2057 GBV_ILN_2061 GBV_ILN_2108 GBV_ILN_2111 GBV_ILN_2119 GBV_ILN_2190 GBV_ILN_4012 GBV_ILN_4037 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4126 GBV_ILN_4249 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_4335 GBV_ILN_4338 GBV_ILN_4367 GBV_ILN_4700 AR 27 2023 1 Part A 207-217 |
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The movement and shape change characteristics of a bubble passing through a liquid-liquid interface |
abstract |
In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. |
abstractGer |
In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. |
abstract_unstemmed |
In order to study the movement and shape change characteristic of bubble when passing through the interface of two kinds of liquids with different viscosity, the free rising process of a single bubble in static stratified liquids was numerically simulated with the volume-of-fluid method. The results show that, when the initial height of bubble rising is the same, the rising velocity, deformation increase with the increase of bubble radius. When the maximum intensity of the vortex in the bubble is distributed at the top of the bubble, the top of the left and right sides and the bottom of the left and right sides, the bubble shape is spherical, ellipsoid and spherical cap shape respectively. At different initial heights, the bubble trajectory shows three different shapes – linear, spiral, and C-shaped. The relation-ship between the bubble aspect ratio and rising height is predicted when different radius bubble passing through the interface. The amount of liquid B (lower layer) carried by the bubble increases with the increase of the bubble’s initial radius, and the amount of liquid carried by bubbles in C-shaped trajectory is higher than that in spiral trajectory. |
collection_details |
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container_issue |
1 Part A |
title_short |
The movement and shape change characteristics of a bubble passing through a liquid-liquid interface |
url |
https://doi.org/10.2298/TSCI220307123X https://doaj.org/article/5f3916ea63b749d5bd438686c7c771df http://www.doiserbia.nb.rs/img/doi/0354-9836/2023/0354-98362200123X.pdf https://doaj.org/toc/0354-9836 https://doaj.org/toc/2334-7163 |
remote_bool |
true |
author2 |
Zhang Xiaohui Qing Shan Wu Jiaying |
author2Str |
Zhang Xiaohui Qing Shan Wu Jiaying |
ppnlink |
514240016 |
callnumber-subject |
TJ - Mechanical Engineering and Machinery |
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doi_str |
10.2298/TSCI220307123X |
callnumber-a |
TJ1-1570 |
up_date |
2024-07-03T15:31:33.275Z |
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