{ "id": "2109.09091", "version": "v1", "published": "2021-09-19T09:16:47.000Z", "updated": "2021-09-19T09:16:47.000Z", "title": "Taylor bubble motion in stagnant and flowing liquids in vertical pipes. Part I: Steady-states", "authors": [ "Habib Abubakar", "Omar Matar" ], "comment": "34 pages, 20 figures", "categories": [ "physics.flu-dyn" ], "abstract": "Taylor bubbles are a feature of the slug flow regime in gas-liquid flows in vertical pipes. Their dynamics exhibits a number of transitions such as symmetry-breaking in the bubble shape and wake when rising in downward-flowing and stagnant liquids, respectively, as well as breakup in sufficiently turbulent environments. Motivated by the need to examine the stability of a Taylor bubble in liquids, a systematic numerical study of a steadily-moving Taylor bubble in stagnant and flowing liquids is carried out, characterised by a dimensionless inverse viscosity ($Nf$), and E\\\"{o}tv\\\"{o}s ($Eo$), and Froude ($Fr$) numbers based on the centreline liquid velocity, using a Galerkin finite-element method. A boundary-fitted domain is used to examine the dependence of the steady bubble shape on a wide range of $Nf$ and $Eo$. Our analysis of the bubble nose and bottom curvatures shows that the intervals $Eo = \\left[ 20,30 \\right)$ and $Nf=\\left[60,80 \\right)$ are the limits below which surface tension and viscosity, respectively, have a strong influence on the bubble shape. In the interval $Eo = \\left(60,100 \\right]$, all bubble features studied are weakly-dependent on surface tension. This is Part I of a two-part publication in which its companion paper (Abubakar & Matar, 2021) reports the results of a linear stability analysis of the steady-states discussed herein.", "revisions": [ { "version": "v1", "updated": "2021-09-19T09:16:47.000Z" } ], "analyses": { "keywords": [ "taylor bubble motion", "flowing liquids", "vertical pipes", "steady-states", "bubble shape" ], "note": { "typesetting": "TeX", "pages": 34, "language": "en", "license": "arXiv", "status": "editable" } } }