Contact Angle Measurement of Liquid Hydrogen (LH2) in Stainless Steel and Aluminum CellsSource: Journal of Heat Transfer:;2016:;volume( 138 ):;issue: 002::page 20904Author: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: 10.1115/1.4032232Publisher: 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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contributor author | Bellur, Kishan | |
contributor author | Konduru, Vinaykumar | |
contributor author | Kulshrestha, Manan | |
contributor author | Tyrewala, Daanish | |
contributor author | Medici, Ezequiel | |
contributor author | Allen, Jeffrey S. | |
contributor author | Choi, Chang Kyoung | |
contributor author | Hussey, Daniel S. | |
contributor author | Jacobson, David C. | |
contributor author | Leأ£o, Juscelino B. | |
contributor author | McQuillen, John | |
contributor author | Hermanson, James | |
contributor author | Tamilarasan, Arun | |
date accessioned | 2017-05-09T01:30:12Z | |
date available | 2017-05-09T01:30:12Z | |
date issued | 2016 | |
identifier issn | 0022-1481 | |
identifier other | ht_138_02_020904.pdf | |
identifier uri | http://yetl.yabesh.ir/yetl/handle/yetl/161547 | |
description 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. | |
publisher | The American Society of Mechanical Engineers (ASME) | |
title | Contact Angle Measurement of Liquid Hydrogen (LH2) in Stainless Steel and Aluminum Cells | |
type | Journal Paper | |
journal volume | 138 | |
journal issue | 2 | |
journal title | Journal of Heat Transfer | |
identifier doi | 10.1115/1.4032232 | |
journal fristpage | 20904 | |
journal lastpage | 20904 | |
identifier eissn | 1528-8943 | |
tree | Journal of Heat Transfer:;2016:;volume( 138 ):;issue: 002 | |
contenttype | Fulltext |