1980
DOI: 10.1016/0021-9797(80)90498-1
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Measuring liquid—liquid interfacial behavior with the deep-channel surface viscometer

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Cited by 16 publications
(3 citation statements)
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“…In order to achieve this condition, inertial effects must be eliminated (see assumption 6) and the effect of contact angle boundary conditions nullified by positioning the interface at a small ledge or knife-edge cut in the wall (Wei and Slattery, 1976;Deemer et al, 1980). 4) There is no mass transfer to or from the gas-liquid interface.…”
Section: Deep Channel Surface Viscometermentioning
confidence: 99%
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“…In order to achieve this condition, inertial effects must be eliminated (see assumption 6) and the effect of contact angle boundary conditions nullified by positioning the interface at a small ledge or knife-edge cut in the wall (Wei and Slattery, 1976;Deemer et al, 1980). 4) There is no mass transfer to or from the gas-liquid interface.…”
Section: Deep Channel Surface Viscometermentioning
confidence: 99%
“…(1971) gave an approximate analysis in which a Powell-Eyring model is used for the interface. Hegde and Slattery (1971;Wei and Slattery, 1976;Deemer et al, 1980;Jiang et al, 1984) I I I I I I I I I I I I I I I I I . I I I I I I apparent surface shear viscosity can be determined from measurements of the velocity distribution in the interface without assuming a specific form for the interfacial stressdeformation behavior.…”
Section: Introductionmentioning
confidence: 99%
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