The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the Process

An inverted bottle empties in a time <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>T</mi><mrow><mi>e</mi><mo>,</mo><mn>0</mn></mrow></ms...

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Main Authors: Callen Schwefler, Peyton Nienaber, Hans C. Mayer
Format: Article
Language:English
Published: MDPI AG 2023-08-01
Series:Fluids
Subjects:
Online Access:https://www.mdpi.com/2311-5521/8/8/225
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author Callen Schwefler
Peyton Nienaber
Hans C. Mayer
author_facet Callen Schwefler
Peyton Nienaber
Hans C. Mayer
author_sort Callen Schwefler
collection DOAJ
description An inverted bottle empties in a time <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>T</mi><mrow><mi>e</mi><mo>,</mo><mn>0</mn></mrow></msub></semantics></math></inline-formula> through a process called “glugging”, whereby gas and liquid compete at the neck (of diameter <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>D</mi><mi>N</mi></msub></semantics></math></inline-formula>). In contrast, an open-top container empties in a much shorter time <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>T</mi><mi>e</mi></msub></semantics></math></inline-formula> through “jetting” due to the lack of gas–liquid competition. Experiments and theory demonstrate that, by introducing a perforation (diameter <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>d</mi><mi>p</mi></msub></semantics></math></inline-formula>), a bottle empties through glugging, jetting, or a combination of the two. For a certain range of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>d</mi><mi>p</mi></msub><mo>/</mo><msub><mi>D</mi><mi>N</mi></msub></mrow></semantics></math></inline-formula>, the perforation increases the emptying time, and a particular value of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>d</mi><mi>p</mi></msub><mo>/</mo><msub><mi>D</mi><mi>N</mi></msub></mrow></semantics></math></inline-formula> is associated with a maximum emptying time <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>T</mi><mrow><mi>e</mi><mo>,</mo><mi>m</mi><mi>a</mi><mi>x</mi></mrow></msub></semantics></math></inline-formula>. We show that the transition from jetting to glugging is initiated by the jet velocity reaching a low threshold, thereby allowing a slug of air entry into the neck that stops jetting and starts the glugging. Once initiated, the glugging proceeds as though there is no perforation. Experimental results covered a range of Eötvös numbers from <i>Eo</i>∼ 20–200 (equivalent to a range of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>D</mi><mi>N</mi></msub><mo>/</mo><msub><mi>L</mi><mi>c</mi></msub><mo>∼</mo></mrow></semantics></math></inline-formula> 4–15, where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>L</mi><mi>c</mi></msub></semantics></math></inline-formula> is the capillary length). The phenomenon of bottle emptying with a perforation adds to the body of bottle literature, which has already considered the influence of shape, inclination, liquid properties, etc.
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spelling doaj.art-fcdf7c0d911548ce9ca1e9ff8d1d06362023-11-19T01:04:40ZengMDPI AGFluids2311-55212023-08-018822510.3390/fluids8080225The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the ProcessCallen Schwefler0Peyton Nienaber1Hans C. Mayer2Department of Mechanical Engineering, California Polytechnic State University, San Luis Obispo, CA 93407, USADepartment of Mechanical Engineering, California Polytechnic State University, San Luis Obispo, CA 93407, USADepartment of Mechanical Engineering, California Polytechnic State University, San Luis Obispo, CA 93407, USAAn inverted bottle empties in a time <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>T</mi><mrow><mi>e</mi><mo>,</mo><mn>0</mn></mrow></msub></semantics></math></inline-formula> through a process called “glugging”, whereby gas and liquid compete at the neck (of diameter <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>D</mi><mi>N</mi></msub></semantics></math></inline-formula>). In contrast, an open-top container empties in a much shorter time <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>T</mi><mi>e</mi></msub></semantics></math></inline-formula> through “jetting” due to the lack of gas–liquid competition. Experiments and theory demonstrate that, by introducing a perforation (diameter <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>d</mi><mi>p</mi></msub></semantics></math></inline-formula>), a bottle empties through glugging, jetting, or a combination of the two. For a certain range of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>d</mi><mi>p</mi></msub><mo>/</mo><msub><mi>D</mi><mi>N</mi></msub></mrow></semantics></math></inline-formula>, the perforation increases the emptying time, and a particular value of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>d</mi><mi>p</mi></msub><mo>/</mo><msub><mi>D</mi><mi>N</mi></msub></mrow></semantics></math></inline-formula> is associated with a maximum emptying time <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>T</mi><mrow><mi>e</mi><mo>,</mo><mi>m</mi><mi>a</mi><mi>x</mi></mrow></msub></semantics></math></inline-formula>. We show that the transition from jetting to glugging is initiated by the jet velocity reaching a low threshold, thereby allowing a slug of air entry into the neck that stops jetting and starts the glugging. Once initiated, the glugging proceeds as though there is no perforation. Experimental results covered a range of Eötvös numbers from <i>Eo</i>∼ 20–200 (equivalent to a range of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>D</mi><mi>N</mi></msub><mo>/</mo><msub><mi>L</mi><mi>c</mi></msub><mo>∼</mo></mrow></semantics></math></inline-formula> 4–15, where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msub><mi>L</mi><mi>c</mi></msub></semantics></math></inline-formula> is the capillary length). The phenomenon of bottle emptying with a perforation adds to the body of bottle literature, which has already considered the influence of shape, inclination, liquid properties, etc.https://www.mdpi.com/2311-5521/8/8/225gluggingjettingair–water flowtwo-phase flowbubble risebottle
spellingShingle Callen Schwefler
Peyton Nienaber
Hans C. Mayer
The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the Process
Fluids
glugging
jetting
air–water flow
two-phase flow
bubble rise
bottle
title The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the Process
title_full The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the Process
title_fullStr The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the Process
title_full_unstemmed The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the Process
title_short The Emptying of a Perforated Bottle: Influence of Perforation Size on Emptying Time and the Physical Nature of the Process
title_sort emptying of a perforated bottle influence of perforation size on emptying time and the physical nature of the process
topic glugging
jetting
air–water flow
two-phase flow
bubble rise
bottle
url https://www.mdpi.com/2311-5521/8/8/225
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