Multistability of a long droplet in a capillary tube under transverse body force
Bistable states for a sufficiently large amount of liquid can appear in an eccentric capillary due to the eccentricity effect under zero gravity (J. Fluid Mech, vol. 863, 2019, pp. 364–385). A transverse body force, which can lead to rich physical phenomena of a droplet, may lead to multistable stat...
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description | Bistable states for a sufficiently large amount of liquid can appear in an eccentric capillary due to the eccentricity effect under zero gravity (J. Fluid Mech, vol. 863, 2019, pp. 364–385). A transverse body force, which can lead to rich physical phenomena of a droplet, may lead to multistable states (bistability, tristability and the likes) of a sufficiently large amount of liquid in a capillary. We theoretically investigate this situation in a circular or annular capillary tube under a transverse body force. The results show that there can be tristable (bistable) states in an annular (circular) capillary tube: an occluding configuration and two (one) non-occluding configurations. In the annular tube, for one of the non-occluding configurations, the gas–liquid interface in the middle cross-section of the droplet meets both the inner and outer walls of the tube (bridging configuration); for the other non-occluding configuration, the gas–liquid interface in the middle cross-section of the droplet does not meet the inner wall (non-bridging configuration). The multistability is dependent on the Bond number, the contact angle and the cross-sectional shape. The multistability cannot occur for a zero or very large Bond number. A hydrophilic condition (the contact angle smaller than 90°) contributes to the non-occluding non-bridging configuration, while the hydrophobic condition (the contact angle larger than 90°) contributes to the non-occluding bridging configuration (only for the annular capillary). For the annular capillary with a not-so-large contact angle, increasing the inner-to-outer radius ratio can lead to a larger range of Bond numbers, in which the multistability occurs. |
doi_str_mv | 10.1017/jfm.2024.689 |
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Fluid Mech, vol. 863, 2019, pp. 364–385). A transverse body force, which can lead to rich physical phenomena of a droplet, may lead to multistable states (bistability, tristability and the likes) of a sufficiently large amount of liquid in a capillary. We theoretically investigate this situation in a circular or annular capillary tube under a transverse body force. The results show that there can be tristable (bistable) states in an annular (circular) capillary tube: an occluding configuration and two (one) non-occluding configurations. In the annular tube, for one of the non-occluding configurations, the gas–liquid interface in the middle cross-section of the droplet meets both the inner and outer walls of the tube (bridging configuration); for the other non-occluding configuration, the gas–liquid interface in the middle cross-section of the droplet does not meet the inner wall (non-bridging configuration). The multistability is dependent on the Bond number, the contact angle and the cross-sectional shape. The multistability cannot occur for a zero or very large Bond number. A hydrophilic condition (the contact angle smaller than 90°) contributes to the non-occluding non-bridging configuration, while the hydrophobic condition (the contact angle larger than 90°) contributes to the non-occluding bridging configuration (only for the annular capillary). For the annular capillary with a not-so-large contact angle, increasing the inner-to-outer radius ratio can lead to a larger range of Bond numbers, in which the multistability occurs.</description><identifier>ISSN: 0022-1120</identifier><identifier>EISSN: 1469-7645</identifier><identifier>DOI: 10.1017/jfm.2024.689</identifier><language>eng</language><publisher>Cambridge, UK: Cambridge University Press</publisher><subject>Bond number ; Bonding ; Capillary tubes ; Configurations ; Contact angle ; Cross-sections ; Droplets ; Equilibrium ; Gravity ; Hydrophobicity ; Investigations ; JFM Papers ; Mathematical models ; Physical phenomena ; Weightlessness</subject><ispartof>Journal of fluid mechanics, 2024-09, Vol.996, Article A28</ispartof><rights>The Author(s), 2024. 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Fluid Mech</addtitle><description>Bistable states for a sufficiently large amount of liquid can appear in an eccentric capillary due to the eccentricity effect under zero gravity (J. Fluid Mech, vol. 863, 2019, pp. 364–385). A transverse body force, which can lead to rich physical phenomena of a droplet, may lead to multistable states (bistability, tristability and the likes) of a sufficiently large amount of liquid in a capillary. We theoretically investigate this situation in a circular or annular capillary tube under a transverse body force. The results show that there can be tristable (bistable) states in an annular (circular) capillary tube: an occluding configuration and two (one) non-occluding configurations. In the annular tube, for one of the non-occluding configurations, the gas–liquid interface in the middle cross-section of the droplet meets both the inner and outer walls of the tube (bridging configuration); for the other non-occluding configuration, the gas–liquid interface in the middle cross-section of the droplet does not meet the inner wall (non-bridging configuration). The multistability is dependent on the Bond number, the contact angle and the cross-sectional shape. The multistability cannot occur for a zero or very large Bond number. A hydrophilic condition (the contact angle smaller than 90°) contributes to the non-occluding non-bridging configuration, while the hydrophobic condition (the contact angle larger than 90°) contributes to the non-occluding bridging configuration (only for the annular capillary). For the annular capillary with a not-so-large contact angle, increasing the inner-to-outer radius ratio can lead to a larger range of Bond numbers, in which the multistability occurs.</description><subject>Bond number</subject><subject>Bonding</subject><subject>Capillary tubes</subject><subject>Configurations</subject><subject>Contact angle</subject><subject>Cross-sections</subject><subject>Droplets</subject><subject>Equilibrium</subject><subject>Gravity</subject><subject>Hydrophobicity</subject><subject>Investigations</subject><subject>JFM Papers</subject><subject>Mathematical models</subject><subject>Physical phenomena</subject><subject>Weightlessness</subject><issn>0022-1120</issn><issn>1469-7645</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNptkE1LxDAQhoMouH7c_AEBr7Zm0jZJj7L4BSt60HNI28mSpdvUJBX239tlF7x4Ghie9x3mIeQGWA4M5P3GbnPOeJkLVZ-QBZSizqQoq1OyYIzzDICzc3IR44YxKFgtF-TjbeqTi8k0rndpR72lhvZ-WNMu-LHHRN0wb1ozur43YUfT1CCdhg4DTcEM8QdDRNr4bketDy1ekTNr-ojXx3lJvp4eP5cv2er9-XX5sMpaUHXKZFHzqi0Mcmw41MCFklhUJWNCKtXUFXZSisIwUxmOrUVTSYYSrTJWgLDFJbk99I7Bf08Yk974KQzzSV0AQKmUkHym7g5UG3yMAa0eg9vOf2hgeu9Mz8703pmenc14fsTNtgmuW-Nf67-BXx4yblg</recordid><startdate>20240930</startdate><enddate>20240930</enddate><creator>Tan, Dongwen</creator><creator>Zhou, Xinping</creator><general>Cambridge University Press</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>7U5</scope><scope>7UA</scope><scope>8FD</scope><scope>C1K</scope><scope>F1W</scope><scope>FR3</scope><scope>H8D</scope><scope>H96</scope><scope>KR7</scope><scope>L.G</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-6340-5273</orcidid><orcidid>https://orcid.org/0000-0002-2205-3045</orcidid></search><sort><creationdate>20240930</creationdate><title>Multistability of a long droplet in a capillary tube under transverse body force</title><author>Tan, Dongwen ; Zhou, Xinping</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c189t-73925c3ae2eb21912687e354006788b95ed7763a0a5a2ecfea570e7ef8af616f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Bond number</topic><topic>Bonding</topic><topic>Capillary tubes</topic><topic>Configurations</topic><topic>Contact angle</topic><topic>Cross-sections</topic><topic>Droplets</topic><topic>Equilibrium</topic><topic>Gravity</topic><topic>Hydrophobicity</topic><topic>Investigations</topic><topic>JFM Papers</topic><topic>Mathematical models</topic><topic>Physical phenomena</topic><topic>Weightlessness</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Tan, Dongwen</creatorcontrib><creatorcontrib>Zhou, Xinping</creatorcontrib><collection>CrossRef</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Water Resources Abstracts</collection><collection>Technology Research Database</collection><collection>Environmental Sciences and Pollution Management</collection><collection>ASFA: Aquatic Sciences and Fisheries Abstracts</collection><collection>Engineering Research Database</collection><collection>Aerospace Database</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) 2: Ocean Technology, Policy & Non-Living Resources</collection><collection>Civil Engineering Abstracts</collection><collection>Aquatic Science & Fisheries Abstracts (ASFA) Professional</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of fluid mechanics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tan, Dongwen</au><au>Zhou, Xinping</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Multistability of a long droplet in a capillary tube under transverse body force</atitle><jtitle>Journal of fluid mechanics</jtitle><addtitle>J. Fluid Mech</addtitle><date>2024-09-30</date><risdate>2024</risdate><volume>996</volume><artnum>A28</artnum><issn>0022-1120</issn><eissn>1469-7645</eissn><abstract>Bistable states for a sufficiently large amount of liquid can appear in an eccentric capillary due to the eccentricity effect under zero gravity (J. Fluid Mech, vol. 863, 2019, pp. 364–385). A transverse body force, which can lead to rich physical phenomena of a droplet, may lead to multistable states (bistability, tristability and the likes) of a sufficiently large amount of liquid in a capillary. We theoretically investigate this situation in a circular or annular capillary tube under a transverse body force. The results show that there can be tristable (bistable) states in an annular (circular) capillary tube: an occluding configuration and two (one) non-occluding configurations. In the annular tube, for one of the non-occluding configurations, the gas–liquid interface in the middle cross-section of the droplet meets both the inner and outer walls of the tube (bridging configuration); for the other non-occluding configuration, the gas–liquid interface in the middle cross-section of the droplet does not meet the inner wall (non-bridging configuration). The multistability is dependent on the Bond number, the contact angle and the cross-sectional shape. The multistability cannot occur for a zero or very large Bond number. A hydrophilic condition (the contact angle smaller than 90°) contributes to the non-occluding non-bridging configuration, while the hydrophobic condition (the contact angle larger than 90°) contributes to the non-occluding bridging configuration (only for the annular capillary). For the annular capillary with a not-so-large contact angle, increasing the inner-to-outer radius ratio can lead to a larger range of Bond numbers, in which the multistability occurs.</abstract><cop>Cambridge, UK</cop><pub>Cambridge University Press</pub><doi>10.1017/jfm.2024.689</doi><tpages>27</tpages><orcidid>https://orcid.org/0000-0001-6340-5273</orcidid><orcidid>https://orcid.org/0000-0002-2205-3045</orcidid></addata></record> |
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subjects | Bond number Bonding Capillary tubes Configurations Contact angle Cross-sections Droplets Equilibrium Gravity Hydrophobicity Investigations JFM Papers Mathematical models Physical phenomena Weightlessness |
title | Multistability of a long droplet in a capillary tube under transverse body force |
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