Rheological and thermal properties of the surface layer of liquids
A grid model of the surface liquid layer at the boundary with the gas and its rheological and thermophysical properties (temperature dependence of the surface tension and surface heat capacity) have been described. It has been obtained that the mole heat capacity of the surface layer is nearly the s...
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| Published in | Journal of engineering physics and thermophysics Vol. 78; no. 5; pp. 1002 - 1005 |
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| Main Author | |
| Format | Journal Article |
| Language | English |
| Published |
Heidelberg
Springer Nature B.V
01.09.2005
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| Subjects | |
| Online Access | Get full text |
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| Abstract | A grid model of the surface liquid layer at the boundary with the gas and its rheological and thermophysical properties (temperature dependence of the surface tension and surface heat capacity) have been described. It has been obtained that the mole heat capacity of the surface layer is nearly the same (5.6 J/(mole·K)) for many liquid metals. It has been shown that for calculation of the rheological properties it is expedient to use the Kelvin model.[PUBLICATION ABSTRACT] |
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| AbstractList | A grid model of the surface liquid layer at the boundary with the gas and its rheological and thermophysical properties (temperature dependence of the surface tension and surface heat capacity) have been described. It has been obtained that the mole heat capacity of the surface layer is nearly the same (5.6 J/(mole·K)) for many liquid metals. It has been shown that for calculation of the rheological properties it is expedient to use the Kelvin model.[PUBLICATION ABSTRACT] A grid model of the surface liquid layer at the boundary with the gas and its rheological and thermophysical properties (temperature dependence of the surface tension and surface heat capacity) have been described. It has been obtained that the mole heat capacity of the surface layer is nearly the same (5.6 J/(mole*K)) for many liquid metals. It has been shown that for calculation of the rheological properties it is expedient to use the Kelvin model. |
| Author | Summ, B D |
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| CitedBy_id | crossref_primary_10_1007_s10008_012_1919_9 crossref_primary_10_1016_j_cis_2010_03_002 crossref_primary_10_1016_j_susc_2009_12_020 |
| Cites_doi | 10.1209/0295-5075/30/5/006 10.1103/PhysRevLett.74.4444 10.1103/PhysRevLett.75.2498 |
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| Copyright | Springer Science+Business Media, Inc. 2005 |
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| References | (26_CR4) 1991 M. Deutsch (26_CR7) 1995; 30 M. J. Regan (26_CR6) 1995; 75 B. D. Summ (26_CR8) 2002; 93 B. D. Summ (26_CR3) 1994; 38 A. I. Rusanov (26_CR9) 1994 J. S. Rowlinson (26_CR1) 1986 B. D. Summ (26_CR2) 1993; 34 O. M. Magnussen (26_CR5) 1995; 74 |
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