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Heat Transfer Research

Published 18 issues per year

ISSN Print: 1064-2285

ISSN Online: 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

Mathematical Simulation of Plasma Expansion in Laser Shock Processing of Materials

Volume 33, Issue 7&8, 2002, 9 pages
DOI: 10.1615/HeatTransRes.v33.i7-8.140
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ABSTRACT

Based on mathematical simulation, investigation of the special features of the expansion and transmission coefficients of an air plasma initiated by an Nd:YAG laser at either l = 1.06 mm (IR action) or l = 0.355 m m (UV action) in the wavelengthm range 1-20 GW /cm2 with a pulse length of 25-30 nsec has been made. The simulation allows one to conclude that the plasma expansion for the IR and UV action is significant1y different. For the IR action the main expansion mechanism is fast propagation of an ionization wave toward the laser source. It is just the ionization wave that absorbs the major part of the laser radiation in this case. For the UV action, the plasma expands as a light-detonation wave, and is mainly influenced by relatively slow gasdynamic processes. The screening effect of the plasma can be characterized by its transmission coefficient. A sharp drop in transmission in 1-2 nsec is observed for the IR action, while for the UV action the decrease is nonmonotonic and takes 10-20 nsec.

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