{"title":"体积守恒法为三维前端跟踪法","authors":"S. Takeuchi, G. Tryggvason","doi":"10.1299/mel.20-00216","DOIUrl":null,"url":null,"abstract":"A method to conserve the volume of dispersed components (e.g. bubbles and droplets) in a viscous fluid is proposed for the front-tracking method (Unverdi and Tryggvason, 1992; Tryggvason et al., 2001). The method adjusts the coordinates of each nodal points on the interface (or Lagrangian markers) along the velocity vector. A simplified algorithm determines the new position of the marker independently from those of the surrounding nodes, which allows the volume correction to be accomplished efficiently. The results show that the volume of a deformed fluid particle is kept constant within errors of O (10 − 7 ) ∼ O (10 − 6 ) . The effects of the time step size and the frequency of the volume correction are investigated. The method is applicable to enclosed structures of non-spherical geometry (e.g. oblate/prolate/spherical-cap fluid particles).","PeriodicalId":180561,"journal":{"name":"Mechanical Engineering Letters","volume":"9 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":"{\"title\":\"Volume conservation method for the three-dimensional front-tracking method\",\"authors\":\"S. Takeuchi, G. Tryggvason\",\"doi\":\"10.1299/mel.20-00216\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"A method to conserve the volume of dispersed components (e.g. bubbles and droplets) in a viscous fluid is proposed for the front-tracking method (Unverdi and Tryggvason, 1992; Tryggvason et al., 2001). The method adjusts the coordinates of each nodal points on the interface (or Lagrangian markers) along the velocity vector. A simplified algorithm determines the new position of the marker independently from those of the surrounding nodes, which allows the volume correction to be accomplished efficiently. The results show that the volume of a deformed fluid particle is kept constant within errors of O (10 − 7 ) ∼ O (10 − 6 ) . The effects of the time step size and the frequency of the volume correction are investigated. The method is applicable to enclosed structures of non-spherical geometry (e.g. oblate/prolate/spherical-cap fluid particles).\",\"PeriodicalId\":180561,\"journal\":{\"name\":\"Mechanical Engineering Letters\",\"volume\":\"9 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1900-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"3\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Mechanical Engineering Letters\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1299/mel.20-00216\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Mechanical Engineering Letters","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1299/mel.20-00216","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
摘要
提出了一种保留粘性流体中分散组分(如气泡和液滴)体积的方法,用于前跟踪方法(Unverdi和Tryggvason, 1992;Tryggvason et al., 2001)。该方法沿速度矢量调整界面上每个节点(或拉格朗日标记)的坐标。一种简化的算法独立于周围节点确定标记点的新位置,从而有效地完成体积校正。结果表明,变形流体颗粒的体积在0(10−7)~ O(10−6)的误差范围内保持恒定。研究了时间步长和体积校正频率的影响。该方法适用于非球面几何的封闭结构(如扁圆/长形/球帽流体颗粒)。
Volume conservation method for the three-dimensional front-tracking method
A method to conserve the volume of dispersed components (e.g. bubbles and droplets) in a viscous fluid is proposed for the front-tracking method (Unverdi and Tryggvason, 1992; Tryggvason et al., 2001). The method adjusts the coordinates of each nodal points on the interface (or Lagrangian markers) along the velocity vector. A simplified algorithm determines the new position of the marker independently from those of the surrounding nodes, which allows the volume correction to be accomplished efficiently. The results show that the volume of a deformed fluid particle is kept constant within errors of O (10 − 7 ) ∼ O (10 − 6 ) . The effects of the time step size and the frequency of the volume correction are investigated. The method is applicable to enclosed structures of non-spherical geometry (e.g. oblate/prolate/spherical-cap fluid particles).