Nang X. Ho, Hoe D. Nguyen, Vinh T. Nguyen, Truong V. Vu
{"title":"Trapping mechanism of a compound droplet on a heterogeneous substrate undergoing the Marangoni effect","authors":"Nang X. Ho, Hoe D. Nguyen, Vinh T. Nguyen, Truong V. Vu","doi":"10.1016/j.geoen.2025.213776","DOIUrl":null,"url":null,"abstract":"<div><div>We numerically study the trapping mechanism of a compound droplet attached to a heterogeneous substrate undergoing the Marangoni effect. The substrate consists of a main part and a wettability-contrasted part. The investigated parameters included <em>Ma</em> (ranging from 0.4 to 0.8), <em>μ</em><sub><em>am</em></sub> (varying from 0.8 to 2.4), <em>R</em><sub><em>io</em></sub> (varying from 0.3 to 0.7), and Δ<em>θ</em><sub><em>e</em></sub> (ranging from 3° to 7°). The droplet becomes trapped at a low value of <em>Ma</em>, <em>μ</em><sub><em>am</em></sub>, and a high value of Δ<em>θ</em><sub><em>e</em></sub> as it moves toward the hot side. When the droplet moves toward the cold side, it becomes trapped at a low value of <em>Ma</em>, but a high value of <em>μ</em><sub><em>am</em></sub> and Δ<em>θ</em><sub><em>e</em></sub>. The inner droplet, in terms of the radius ratio <em>R</em><sub><em>io</em></sub>, has a significant impact on the trapping behavior of the outer droplet. Interestingly, the compound droplet with <em>R</em><sub><em>io</em></sub>≤ 0.3 crosses the wettability-contrasted part more easily the one with <em>R</em><sub><em>io</em></sub> = 0.4. In addition, when migrating toward the hot side, the compound droplet with a large contact angle allowing a larger inner droplet (0.5 ≤ <em>R</em><sub><em>io</em></sub> ≤ 0.7) is pulled across the wettability-contrasted part by the inner droplet as <em>Ma</em> ≥ 0.5. The trapping behavior rarely occurs in this case. Phase diagrams showing the transition between the trapping and passing behaviors are also proposed.</div></div>","PeriodicalId":100578,"journal":{"name":"Geoenergy Science and Engineering","volume":"249 ","pages":"Article 213776"},"PeriodicalIF":0.0000,"publicationDate":"2025-02-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Geoenergy Science and Engineering","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S2949891025001344","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"0","JCRName":"ENERGY & FUELS","Score":null,"Total":0}
引用次数: 0
Abstract
We numerically study the trapping mechanism of a compound droplet attached to a heterogeneous substrate undergoing the Marangoni effect. The substrate consists of a main part and a wettability-contrasted part. The investigated parameters included Ma (ranging from 0.4 to 0.8), μam (varying from 0.8 to 2.4), Rio (varying from 0.3 to 0.7), and Δθe (ranging from 3° to 7°). The droplet becomes trapped at a low value of Ma, μam, and a high value of Δθe as it moves toward the hot side. When the droplet moves toward the cold side, it becomes trapped at a low value of Ma, but a high value of μam and Δθe. The inner droplet, in terms of the radius ratio Rio, has a significant impact on the trapping behavior of the outer droplet. Interestingly, the compound droplet with Rio≤ 0.3 crosses the wettability-contrasted part more easily the one with Rio = 0.4. In addition, when migrating toward the hot side, the compound droplet with a large contact angle allowing a larger inner droplet (0.5 ≤ Rio ≤ 0.7) is pulled across the wettability-contrasted part by the inner droplet as Ma ≥ 0.5. The trapping behavior rarely occurs in this case. Phase diagrams showing the transition between the trapping and passing behaviors are also proposed.