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    Contact Angle Measurement of Liquid Hydrogen (LH2) in Stainless Steel and Aluminum Cells

    Source: Journal of Heat Transfer:;2016:;volume( 138 ):;issue: 002::page 20904
    Author:
    Bellur, Kishan
    ,
    Konduru, Vinaykumar
    ,
    Kulshrestha, Manan
    ,
    Tyrewala, Daanish
    ,
    Medici, Ezequiel
    ,
    Allen, Jeffrey S.
    ,
    Choi, Chang Kyoung
    ,
    Hussey, Daniel S.
    ,
    Jacobson, David C.
    ,
    Leأ£o, Juscelino B.
    ,
    McQuillen, John
    ,
    Hermanson, James
    ,
    Tamilarasan, Arun
    DOI: 10.1115/1.4032232
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: One of the key limitations to longterm space missions is to avoid propellant boiloff in a microgravity space environment. Even with the use of active and passive controls of propellants, boil off is inevitable. Longterm CFD simulations on propellant behaviors depend on evaporation/condensation coefficients (known as accommodation coefficients) which are in turn dependent upon the wetting characteristics. Phase change experiments were conducted in the BT2 neutron imaging facility at the National Institute of Standards and Technology (NIST) by introducing vapor H2 in 10 mm Al6061 and SS316L test cells placed inside the 70mm â€کorange’ cryostat. Condensation is achieved by lowering the cryostat temperature below the saturation point and vice versa for evaporation. The high neutron crosssection of liquid H2 in comparison to both the vapor and the test cell materials allows for visualization of a distinct liquidvapor interface. Multiple images are stacked to increase the signaltonoise ratio and the meniscus edge is obtained by detecting the pixels with largest gradients in intensities at the liquid meniscus. The contact angle is obtained by curve fitting of the YoungLaplace equation to the detected meniscus. The contact angle for Al6061 and SS316 is found to be between 0آ° and 4آ°. The uncertainty arises from edge detection, magnification, and resolution limits of the neutron imaging setup. The test was conducted at a saturation temperature of 21K (1.215 bar). The results from the neutron experiments will be then used in conjunction with FEA thermal models and kinetic phase change models to extract accommodation coefficients.
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      Contact Angle Measurement of Liquid Hydrogen (LH2) in Stainless Steel and Aluminum Cells

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    http://yetl.yabesh.ir/yetl1/handle/yetl/161547
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    contributor authorBellur, Kishan
    contributor authorKonduru, Vinaykumar
    contributor authorKulshrestha, Manan
    contributor authorTyrewala, Daanish
    contributor authorMedici, Ezequiel
    contributor authorAllen, Jeffrey S.
    contributor authorChoi, Chang Kyoung
    contributor authorHussey, Daniel S.
    contributor authorJacobson, David C.
    contributor authorLeأ£o, Juscelino B.
    contributor authorMcQuillen, John
    contributor authorHermanson, James
    contributor authorTamilarasan, Arun
    date accessioned2017-05-09T01:30:12Z
    date available2017-05-09T01:30:12Z
    date issued2016
    identifier issn0022-1481
    identifier otherht_138_02_020904.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/161547
    description abstractOne of the key limitations to longterm space missions is to avoid propellant boiloff in a microgravity space environment. Even with the use of active and passive controls of propellants, boil off is inevitable. Longterm CFD simulations on propellant behaviors depend on evaporation/condensation coefficients (known as accommodation coefficients) which are in turn dependent upon the wetting characteristics. Phase change experiments were conducted in the BT2 neutron imaging facility at the National Institute of Standards and Technology (NIST) by introducing vapor H2 in 10 mm Al6061 and SS316L test cells placed inside the 70mm â€کorange’ cryostat. Condensation is achieved by lowering the cryostat temperature below the saturation point and vice versa for evaporation. The high neutron crosssection of liquid H2 in comparison to both the vapor and the test cell materials allows for visualization of a distinct liquidvapor interface. Multiple images are stacked to increase the signaltonoise ratio and the meniscus edge is obtained by detecting the pixels with largest gradients in intensities at the liquid meniscus. The contact angle is obtained by curve fitting of the YoungLaplace equation to the detected meniscus. The contact angle for Al6061 and SS316 is found to be between 0آ° and 4آ°. The uncertainty arises from edge detection, magnification, and resolution limits of the neutron imaging setup. The test was conducted at a saturation temperature of 21K (1.215 bar). The results from the neutron experiments will be then used in conjunction with FEA thermal models and kinetic phase change models to extract accommodation coefficients.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleContact Angle Measurement of Liquid Hydrogen (LH2) in Stainless Steel and Aluminum Cells
    typeJournal Paper
    journal volume138
    journal issue2
    journal titleJournal of Heat Transfer
    identifier doi10.1115/1.4032232
    journal fristpage20904
    journal lastpage20904
    identifier eissn1528-8943
    treeJournal of Heat Transfer:;2016:;volume( 138 ):;issue: 002
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
    yabeshDSpacePersian