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Volumn 20, Issue 7, 2004, Pages 2726-2729

Analysis of pseudopartial and partial wetting of various substrates by lead

Author keywords

[No Author keywords available]

Indexed keywords

CAPILLARITY; CONTACT ANGLE; DROP FORMATION; FREE ENERGY; INTERFACIAL ENERGY; ISOTHERMS; PHASE EQUILIBRIA; SUBSTRATES; WETTING;

EID: 1842759875     PISSN: 07437463     EISSN: None     Source Type: Journal    
DOI: 10.1021/la035759d     Document Type: Article
Times cited : (9)

References (32)
  • 3
    • 0002610943 scopus 로고
    • Thermodynamics of thin films and three-phase contact regions
    • Morrow, N., Ed.; Marcel Dekker: New York
    • Hirasaki, G. Thermodynamics of Thin Films and Three-Phase Contact Regions. In Interfacial Phenomena in Petroleum Recovery; Morrow, N., Ed.; Marcel Dekker: New York, 1991.
    • (1991) Interfacial Phenomena in Petroleum Recovery
    • Hirasaki, G.1
  • 4
    • 0039316382 scopus 로고
    • Shape of meniscus/film transition region
    • Morrow, N., Ed.; Marcel Dekker: New York
    • Hirasaki, G. Shape of Meniscus/Film Transition Region. In Interfacial Phenomena in Petroleum Recovery; Morrow, N., Ed.; Marcel Dekker: New York, 1991.
    • (1991) Interfacial Phenomena in Petroleum Recovery
    • Hirasaki, G.1
  • 5
    • 0027856990 scopus 로고
    • Sharma, A. Langmuir 1993, 9, 3580-3586.
    • (1993) Langmuir , vol.9 , pp. 3580-3586
    • Sharma, A.1
  • 12
    • 1842627720 scopus 로고    scopus 로고
    • Wetting and energies of metal/SiC and metal/graphite interfaces
    • Ph.D. Thesis, Carnegie Mellon University, Pittsburgh, PA
    • Wang,Z. Wetting and Energies of Metal/SiC and Metal/Graphite Interfaces. Ph.D. Thesis, Carnegie Mellon University, Pittsburgh, PA, 1998.
    • (1998)
    • Wang, Z.1
  • 15
    • 1842627722 scopus 로고    scopus 로고
    • note
    • The film coverage h is the number of monolayers of lead covering the solid surface. This designation allows h to vary continuously from a bare substrate to the thickness of macroscopically thick films.
  • 16
    • 1842728487 scopus 로고    scopus 로고
    • note
    • Since the cohesive energy of lead (ref 32) is approximately 58 kT in the conditions of these experiments, the rate of evaporation from the drop into the vapor is negligibly small. Evaporated atoms did not recondense on the sample since these experiments were conducted in a UHV chamber where the mean free path between collisions of evaporated lead atoms was much larger than the chamber size and where the chamber walls were cool enough to trap the ballistic evaporated lead atoms.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.