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ISSN 打印: 1064-2285

ISSN 在线: 2162-6561

The Impact Factor measures the average number of citations received in a particular year by papers published in the journal during the two preceding years. 2017 Journal Citation Reports (Clarivate Analytics, 2018) IF: 1.7 To calculate the five year Impact Factor, citations are counted in 2017 to the previous five years and divided by the source items published in the previous five years. 2017 Journal Citation Reports (Clarivate Analytics, 2018) 5-Year IF: 1.4 The Immediacy Index is the average number of times an article is cited in the year it is published. The journal Immediacy Index indicates how quickly articles in a journal are cited. Immediacy Index: 0.6 The Eigenfactor score, developed by Jevin West and Carl Bergstrom at the University of Washington, is a rating of the total importance of a scientific journal. Journals are rated according to the number of incoming citations, with citations from highly ranked journals weighted to make a larger contribution to the eigenfactor than those from poorly ranked journals. Eigenfactor: 0.00072 The Journal Citation Indicator (JCI) is a single measurement of the field-normalized citation impact of journals in the Web of Science Core Collection across disciplines. The key words here are that the metric is normalized and cross-disciplinary. JCI: 0.43 SJR: 0.318 SNIP: 0.568 CiteScore™:: 3.5 H-Index: 28

Indexed in

EFFECT OF CORRUGATION HEIGHT ON FLOW AND HEAT TRANSFER MECHANISM IN A CORRUGATION CHANNEL

卷 50, 册 13, 2019, pp. 1231-1249
DOI: 10.1615/HeatTransRes.2018027243
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摘要

The purpose of the present study is to assess the fl ow and heat transfer performance of a corrugation channel considering various corrugation heights. Furthermore, heat transfer enhancement mechanism is revealed. The results show that the Nusselt number off ered by a corrugation channel with H = 3, 4.5, and 6 mm is equal to around 41.89 to 123.07, 55.56 to 150.02, and 72.18 to 175. The Nusselt number with H = 6 mm is 42−72% higher than that with H = 3 mm. The results show that two peak values exist near the entrance and exit along the concave wall. Thus, a peak value and the lowest point appear near the entrance and the exit along the convex wall. Fluid recirculation zones are generated upstream of the concave wall and downstream of the convex wall. The thermal boundary layer becomes thinnest downstream of the corrugation for the concave wall and near the entrance of the corrugation for the convex wall. Moreover, the highest level of TKE concentrates on the convex wall.

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