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The Journal of Chemical Physics
Volumn 67, Issue 11, 1977, Pages 4850-4857
Dielectric dispersion and dielectric friction in electrolyte solutions. I
Author keywords

[No Author keywords available]
Indexed keywords

EID: 4243207639     PISSN: 00219606     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.434664     Document Type: Article
Times cited : (483)
References (24)
  • 11
    • 85034682101 scopus 로고    scopus 로고
    • therefore vanishes identically for [formula omitted] where a and b are constant vectors
    • F
  • 12
    • 84950874032 scopus 로고    scopus 로고
    • This form insures the local conservation of angular momentum. Incidentally, M. Born’s stress tensor is not symmetric, and he seemed to be aware of the implications, but apparently he was unable to remedy the situation.
  • 17
    • 85034675751 scopus 로고    scopus 로고
    • This integral is most conveniently evaluated in a coordinate system moving with the ion, so that the equipotential boundary planes move at the steady velocity u. The equipotential condition on the boundary surfaces implies that the total induced image charge is the negative of the ion charge.
  • 18
    • 85034675990 scopus 로고    scopus 로고
    • Therefore, the frictional drag on a point charge is proportional to the square root of charge and the 3/4 power of solvent viscosity.
  • 22
    • 85034674857 scopus 로고    scopus 로고
    • Here solvation refers to the “firm” attachment of solvent molecules to the ion, so that these molecules take no part in the hydrodynamic motion of the fluid.
  • 24
    • 84950846078 scopus 로고    scopus 로고
    • If we allow for viscous relaxation, then even in the absence of dielectric friction the dispersion will have a pole located at [formula omitted] in addition to the Debye pole.

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.