The heat transfer coefficient spatial distribution reconstruction by an inverse technique
This article presents a technique for obtaining the spatial distribution of the heat transfer coefficient (HTC) for an impingement heat exchange directly from transient temperature measurements. The HTC retrieval problem is formulated through the boundary temperature and the heat flux. That formulat...
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Published in | Inverse problems in science and engineering Vol. 19; no. 1; pp. 117 - 126 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Taylor & Francis
01.01.2011
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Abstract | This article presents a technique for obtaining the spatial distribution of the heat transfer coefficient (HTC) for an impingement heat exchange directly from transient temperature measurements. The HTC retrieval problem is formulated through the boundary temperature and the heat flux. That formulation makes it possible to utilize the superposition principle as the temperature field depends linearly on both the mentioned boundary conditions (BC). The unknown boundary temperature and heat flux are approximated by the set of trial functions chosen by the user. The key point is to utilize the definition of the convective BC in the objective function formulation. This fact allows us to take advantage of the fact that for the impingement heat exchange the HTC is constant in time. Such definition of the minimized function improves the stability of the solution in the presence of the measurement errors. |
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AbstractList | This article presents a technique for obtaining the spatial distribution of the heat transfer coefficient (HTC) for an impingement heat exchange directly from transient temperature measurements. The HTC retrieval problem is formulated through the boundary temperature and the heat flux. That formulation makes it possible to utilize the superposition principle as the temperature field depends linearly on both the mentioned boundary conditions (BC). The unknown boundary temperature and heat flux are approximated by the set of trial functions chosen by the user. The key point is to utilize the definition of the convective BC in the objective function formulation. This fact allows us to take advantage of the fact that for the impingement heat exchange the HTC is constant in time. Such definition of the minimized function improves the stability of the solution in the presence of the measurement errors. |
Author | Bialecki, R. Ryfa, A. |
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CitedBy_id | crossref_primary_10_1080_10407782_2012_657998 crossref_primary_10_1016_j_applthermaleng_2018_09_085 crossref_primary_10_1016_j_ijheatfluidflow_2011_06_005 crossref_primary_10_1080_10407782_2013_807669 crossref_primary_10_1088_0266_5611_29_9_095020 crossref_primary_10_1115_1_4047146 |
Cites_doi | 10.1016/j.ijheatmasstransfer.2007.01.044 10.1016/j.ijheatmasstransfer.2006.03.034 10.1016/j.ijrefrig.2005.05.016 10.1080/17415970902888400 10.1002/nme.671 10.1115/1.2910554 |
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SubjectTerms | Boundaries boundary conditions Formulations Heat exchange Heat flux Heat transfer Heat transfer coefficients Impingement impingement cooling inverse analysis Spatial distribution |
Title | The heat transfer coefficient spatial distribution reconstruction by an inverse technique |
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