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    Effervescent Atomization of Viscoelastic Liquids: Experiment and Modeling

    Source: Journal of Fluids Engineering:;2008:;volume( 130 ):;issue: 006::page 61303
    Author:
    S. C. Geckler
    ,
    P. E. Sojka
    DOI: 10.1115/1.2917430
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: The effervescent atomization of viscoelastic liquids is reported. A total of 23 fluids, formulated from a 60wt% glycerine/40wt% water solvent to which were added varying concentrations (0.001–0.5wt%) of poly(ethylene oxide) polymers whose molecular weights ranged from 12,000 to 900,000, were sprayed through a conventional effervescent atomizer. Mean drop sizes were measured using a forward light scattering instrument. The drop size (D32) data show the expected decrease with an increase in air-liquid ratio by mass (ALR), the expected increase with an increase in polymer concentration, plus an increase with an increase in polymer molecular weight for most cases. However, no significant change in D32 was observed for polymer solutions whose molecular weights ranged from 12,000 to 35,000, suggesting the presence of a critical molecular weight below which spray performance is unaltered. This argues for two different factors controlling drop size: Polymer molecular weight is most influential at the highest polymer concentrations while polymer concentration is most influential at the lowest polymer concentrations. Analysis of the spray formation process was carried out using a ligament formation model previously developed for the effervescent atomization of Newtonian liquids coupled with a linear stability model for the breakup of viscoelastic liquid jets. The jet breakup model assumes that an unrelaxed axial tension exists within the fluid. A comparison of model predictions and experimental data indicates that the model predicts the observed dependencies of mean drop size on ALR, polymer concentration, and polymer molecular weight. Quantitative agreement is within 10–50% of experimental values in all cases. Finally, a shortcoming of the model is noted and a means of avoiding this limitation reported.
    keyword(s): Fluids , Drops , Polymers , Sprays , Molecular weight , Water , Stability AND Tension ,
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      Effervescent Atomization of Viscoelastic Liquids: Experiment and Modeling

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    http://yetl.yabesh.ir/yetl1/handle/yetl/138224
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    • Journal of Fluids Engineering

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    contributor authorS. C. Geckler
    contributor authorP. E. Sojka
    date accessioned2017-05-09T00:28:26Z
    date available2017-05-09T00:28:26Z
    date copyrightJune, 2008
    date issued2008
    identifier issn0098-2202
    identifier otherJFEGA4-27318#061303_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/138224
    description abstractThe effervescent atomization of viscoelastic liquids is reported. A total of 23 fluids, formulated from a 60wt% glycerine/40wt% water solvent to which were added varying concentrations (0.001–0.5wt%) of poly(ethylene oxide) polymers whose molecular weights ranged from 12,000 to 900,000, were sprayed through a conventional effervescent atomizer. Mean drop sizes were measured using a forward light scattering instrument. The drop size (D32) data show the expected decrease with an increase in air-liquid ratio by mass (ALR), the expected increase with an increase in polymer concentration, plus an increase with an increase in polymer molecular weight for most cases. However, no significant change in D32 was observed for polymer solutions whose molecular weights ranged from 12,000 to 35,000, suggesting the presence of a critical molecular weight below which spray performance is unaltered. This argues for two different factors controlling drop size: Polymer molecular weight is most influential at the highest polymer concentrations while polymer concentration is most influential at the lowest polymer concentrations. Analysis of the spray formation process was carried out using a ligament formation model previously developed for the effervescent atomization of Newtonian liquids coupled with a linear stability model for the breakup of viscoelastic liquid jets. The jet breakup model assumes that an unrelaxed axial tension exists within the fluid. A comparison of model predictions and experimental data indicates that the model predicts the observed dependencies of mean drop size on ALR, polymer concentration, and polymer molecular weight. Quantitative agreement is within 10–50% of experimental values in all cases. Finally, a shortcoming of the model is noted and a means of avoiding this limitation reported.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleEffervescent Atomization of Viscoelastic Liquids: Experiment and Modeling
    typeJournal Paper
    journal volume130
    journal issue6
    journal titleJournal of Fluids Engineering
    identifier doi10.1115/1.2917430
    journal fristpage61303
    identifier eissn1528-901X
    keywordsFluids
    keywordsDrops
    keywordsPolymers
    keywordsSprays
    keywordsMolecular weight
    keywordsWater
    keywordsStability AND Tension
    treeJournal of Fluids Engineering:;2008:;volume( 130 ):;issue: 006
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
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