A lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance

In a theoretical analysis, a lump-integral model for freezing and melting of the bath material onto a cylindrical additive having its thermal resistance negligible with respect to that of the bath is developed. It is regulated by independent nondimensional parameters, namely the Stefan numb...

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Main Authors: Singh U.C., Prasad A., Kumar A.
Format: Article
Language:English
Published: University of Belgrade, Technical Faculty, Bor 2013-01-01
Series:Journal of Mining and Metallurgy. Section B: Metallurgy
Subjects:
Online Access:http://www.doiserbia.nb.rs/img/doi/1450-5339/2013/1450-53391300028S.pdf
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author Singh U.C.
Prasad A.
Kumar A.
author_facet Singh U.C.
Prasad A.
Kumar A.
author_sort Singh U.C.
collection DOAJ
description In a theoretical analysis, a lump-integral model for freezing and melting of the bath material onto a cylindrical additive having its thermal resistance negligible with respect to that of the bath is developed. It is regulated by independent nondimensional parameters, namely the Stefan number, St the heat capacity ratio, Cr and the modified conduction factor, Cofm. Series solutions associated with short times for time variant growth of the frozen layer and rise in interface temperature between the additive and the frozen layer are obtained. For all times, numerical solutions concerning the frozen layer growth with its melting and increase in the interface temperature are also found. Time for freezing and melting is estimated for different values of Cr, St and Cofm. It is predicted that for lower total time of freezing and melting Cofm<2 or Cr<1 needs to be maintained. When the bath temperature equals the freezing temperature of the bath material, the model is governed by only Cr and St and gives closed-form expressions for the growth of the frozen layer and the interface temperature. For the interface attaining the freezing temperature of the bath material the maximum thickness of the frozen layer becomes ξmax-√Cr(Cr+St). The model is validated once it is reduced to a problem of heating of the additive without freezing of the bath material onto the additive. Its closed-form solution is exactly the same as that reported in the literature.
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record_format Article
series Journal of Mining and Metallurgy. Section B: Metallurgy
spelling doaj-art-cbedf7ac0c024ac2a27246592eea2c162025-02-02T23:57:13ZengUniversity of Belgrade, Technical Faculty, BorJournal of Mining and Metallurgy. Section B: Metallurgy1450-53392013-01-0149324525610.2298/JMMB120808028S1450-53391300028SA lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistanceSingh U.C.0Prasad A.1Kumar A.2Engineering Division, Tata Steel Limited, Business centre, Bistupur, Jamshedpur, IndiaDepartment of Mechanical Engineering, National Institute of Technology, Jamshedpur, IndiaDepartment of Mechanical Engineering, Birla institute of Technology Mesra, Ranchi, IndiaIn a theoretical analysis, a lump-integral model for freezing and melting of the bath material onto a cylindrical additive having its thermal resistance negligible with respect to that of the bath is developed. It is regulated by independent nondimensional parameters, namely the Stefan number, St the heat capacity ratio, Cr and the modified conduction factor, Cofm. Series solutions associated with short times for time variant growth of the frozen layer and rise in interface temperature between the additive and the frozen layer are obtained. For all times, numerical solutions concerning the frozen layer growth with its melting and increase in the interface temperature are also found. Time for freezing and melting is estimated for different values of Cr, St and Cofm. It is predicted that for lower total time of freezing and melting Cofm<2 or Cr<1 needs to be maintained. When the bath temperature equals the freezing temperature of the bath material, the model is governed by only Cr and St and gives closed-form expressions for the growth of the frozen layer and the interface temperature. For the interface attaining the freezing temperature of the bath material the maximum thickness of the frozen layer becomes ξmax-√Cr(Cr+St). The model is validated once it is reduced to a problem of heating of the additive without freezing of the bath material onto the additive. Its closed-form solution is exactly the same as that reported in the literature.http://www.doiserbia.nb.rs/img/doi/1450-5339/2013/1450-53391300028S.pdfadditive additionmelt-additive systemmathematical modelingfreezing and melting
spellingShingle Singh U.C.
Prasad A.
Kumar A.
A lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance
Journal of Mining and Metallurgy. Section B: Metallurgy
additive addition
melt-additive system
mathematical modeling
freezing and melting
title A lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance
title_full A lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance
title_fullStr A lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance
title_full_unstemmed A lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance
title_short A lump-integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance
title_sort lump integral model based freezing and melting of a bath material onto a cylindrical additive of negligible resistance
topic additive addition
melt-additive system
mathematical modeling
freezing and melting
url http://www.doiserbia.nb.rs/img/doi/1450-5339/2013/1450-53391300028S.pdf
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