2017
DOI: 10.1103/physrevfluids.2.023301
|View full text |Cite
|
Sign up to set email alerts
|

Pressure-dependent surface viscosity and its surprising consequences in interfacial lubrication flows

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
38
0

Year Published

2017
2017
2022
2022

Publication Types

Select...
6

Relationship

1
5

Authors

Journals

citations
Cited by 18 publications
(40 citation statements)
references
References 49 publications
1
38
0
Order By: Relevance
“…The effect of Π -dependent rheology is, therefore, more prominent as the fluid film between surface layers becomes thinner. Within this thin layer, a Π -dependent lubrication analysis [29] is possible, which, as we show in §3c, retrieves the same limiting behaviour as equation (3.9). The complementary case of a disc approaching (or departing) a wall along the y-direction is amenable to a simple symmetry argument.…”
Section: Cylinder Next To a Plane Wall (A) Translationsupporting
confidence: 53%
See 3 more Smart Citations
“…The effect of Π -dependent rheology is, therefore, more prominent as the fluid film between surface layers becomes thinner. Within this thin layer, a Π -dependent lubrication analysis [29] is possible, which, as we show in §3c, retrieves the same limiting behaviour as equation (3.9). The complementary case of a disc approaching (or departing) a wall along the y-direction is amenable to a simple symmetry argument.…”
Section: Cylinder Next To a Plane Wall (A) Translationsupporting
confidence: 53%
“…We have previously established the surprising consequences of Π -dependent viscosity in small fluid gaps [29], for any form of η s (Π ) and arbitrary velocities. The current work, on the other hand, focuses on 'small' velocities in a perturbative sense, without restrictions on the thickness of the fluid gap.…”
Section: Resultsmentioning
confidence: 97%
See 2 more Smart Citations
“…For Manifold B and C we use r(θ, φ) = 1 + r 0 sin(3φ) cos(θ) (Manifold B), r(θ, φ) = 1 + r 0 sin(7φ) cos(θ) (Manifold C). (60) Additional details concerning the differential geometry of these radial manifolds can be found in our prior work [35] and in Appendix B and C. Figure 9: Radial Manifold Shapes. We consider hydrodynamic flows on manifolds with shapes ranging from the sphere to the more complicated geometries generated by equation 60.…”
Section: Hydrodynamic Flows On Curved Fluid Interfacesmentioning
confidence: 99%