Moving contact lines and rivulet instabilities. Part 1. The static rivulet
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...S models simultaneously trying to point out their common or specific features (Dussan V. 1976; Huh & Mason 1977b; Davis 1980; Zhou & Sheng 1990; Haley & Miksis 1991) or use purely empirical approaches (Kafka & Dussan V. 1979; Ngan & Dussan V. 1989; Dussan V. et al. 1991)....
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...…boundary condition (Lamb 1932, p. 586), where for the coefficient of sliding friction one may use (S1a) β = const (Hocking 1977, 1981, 1990, 1992; Huh & Mason 1977b; Davis 1980; Lowndes 1980; Levine et al. 1980; Hocking & Rivers 1982; Zhou & Sheng 1990; Ehrhard & Davis 1991; Haley & Miksis 1991)....
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...1976; Hocking 1977, 1981, 1992; Huh & Mason 1977b; Davis 1980; Hocking & Rivers 1982; Cox 1986; Durbin 1988; Zhou & Sheng 1990) (A2) U = k(θd−θs), where k is an empirical constant (Greenspan 1978; Greenspan & McCay 1981; Davis 1980; Hocking 1990; Haley & Miksis 1991)....
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...586), where for the coefficient of sliding friction one may use (S1a) β = const (Hocking 1977, 1981, 1990, 1992; Huh & Mason 1977b; Davis 1980; Lowndes 1980; Levine et al. 1980; Hocking & Rivers 1982; Zhou & Sheng 1990; Ehrhard & Davis 1991; Haley & Miksis 1991)....
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...…devoted to the subject, one can find the following approaches to Problem A: (A1) θd ≡ θs (Dussan V. 1976; Hocking 1977, 1981, 1992; Huh & Mason 1977b; Davis 1980; Hocking & Rivers 1982; Cox 1986; Durbin 1988; Zhou & Sheng 1990) (A2) U = k(θd−θs), where k is an empirical constant (Greenspan 1978;…...
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