Centrifugally forced Rayleigh-Taylor instability
We consider the effect of high rotation rates on two liquid layers that initially form concentric cylinders, centred on the axis of rotation. The configuration may be thought of as a fluid-fluid centrifuge. There are two types of perturbation to the interface that may be considered, an azimuthal pe...
| Main Authors: | , |
|---|---|
| Format: | Article |
| Published: |
Cambridge University Press
2018
|
| Online Access: | https://eprints.nottingham.ac.uk/52611/ |
| _version_ | 1848798767261679616 |
|---|---|
| author | Scase, Matthew M. Hill, Richard J.A. |
| author_facet | Scase, Matthew M. Hill, Richard J.A. |
| author_sort | Scase, Matthew M. |
| building | Nottingham Research Data Repository |
| collection | Online Access |
| description | We consider the effect of high rotation rates on two liquid layers that initially form concentric cylinders, centred on the axis of rotation. The configuration may be thought of as a fluid-fluid centrifuge. There are two types of perturbation to the interface that may be considered, an azimuthal perturbation around the circumference of the interface and a varicose perturbation in the axial direction along the length of the interface. It is the first of these types of perturbation that we consider here, and so the flow may be considered essentially two-dimensional, taking place in a circular domain.
A linear stability analysis is carried out on a perturbation to the hydrostatic background state and a fourth order Orr-Sommerfeld-like equation that governs the system is derived. We consider the dynamics of systems of stable and unstable configurations, inviscid and viscous fluids, immiscible fluid layers with surface tension, and miscible fluid layers that may have some initial diffusion of density. In the most simple case of two layers of inviscid fluid separated by a sharp interface with no surface tension acting, we show that the effects of the curvature of the interface and the confinement of the system may be characterized by a modified Atwood number. The classical Atwood number is recovered in the limit of high azimuthal wavenumber, or the outer fluid layer being unconfined. Theoretical predictions are compared with numerical experiments and the agreement is shown to be good. We do not restrict our analysis to equal volume fluid layers and so our results also have applications in coating and lubrication problems in rapidly rotating systems and machinery. |
| first_indexed | 2025-11-14T20:25:00Z |
| format | Article |
| id | nottingham-52611 |
| institution | University of Nottingham Malaysia Campus |
| institution_category | Local University |
| last_indexed | 2025-11-14T20:25:00Z |
| publishDate | 2018 |
| publisher | Cambridge University Press |
| recordtype | eprints |
| repository_type | Digital Repository |
| spelling | nottingham-526112020-05-04T19:42:21Z https://eprints.nottingham.ac.uk/52611/ Centrifugally forced Rayleigh-Taylor instability Scase, Matthew M. Hill, Richard J.A. We consider the effect of high rotation rates on two liquid layers that initially form concentric cylinders, centred on the axis of rotation. The configuration may be thought of as a fluid-fluid centrifuge. There are two types of perturbation to the interface that may be considered, an azimuthal perturbation around the circumference of the interface and a varicose perturbation in the axial direction along the length of the interface. It is the first of these types of perturbation that we consider here, and so the flow may be considered essentially two-dimensional, taking place in a circular domain. A linear stability analysis is carried out on a perturbation to the hydrostatic background state and a fourth order Orr-Sommerfeld-like equation that governs the system is derived. We consider the dynamics of systems of stable and unstable configurations, inviscid and viscous fluids, immiscible fluid layers with surface tension, and miscible fluid layers that may have some initial diffusion of density. In the most simple case of two layers of inviscid fluid separated by a sharp interface with no surface tension acting, we show that the effects of the curvature of the interface and the confinement of the system may be characterized by a modified Atwood number. The classical Atwood number is recovered in the limit of high azimuthal wavenumber, or the outer fluid layer being unconfined. Theoretical predictions are compared with numerical experiments and the agreement is shown to be good. We do not restrict our analysis to equal volume fluid layers and so our results also have applications in coating and lubrication problems in rapidly rotating systems and machinery. Cambridge University Press 2018-10-10 Article PeerReviewed Scase, Matthew M. and Hill, Richard J.A. (2018) Centrifugally forced Rayleigh-Taylor instability. Journal of Fluid Mechanics, 852 . pp. 543-577. ISSN 1469-7645 https://www.cambridge.org/core/journals/journal-of-fluid-mechanics/article/centrifugally-forced-rayleightaylor-instability/D4642D283F5C8CF794ADAAB5E4510D0B doi:10.1017/jfm.2018.539 doi:10.1017/jfm.2018.539 |
| spellingShingle | Scase, Matthew M. Hill, Richard J.A. Centrifugally forced Rayleigh-Taylor instability |
| title | Centrifugally forced Rayleigh-Taylor instability |
| title_full | Centrifugally forced Rayleigh-Taylor instability |
| title_fullStr | Centrifugally forced Rayleigh-Taylor instability |
| title_full_unstemmed | Centrifugally forced Rayleigh-Taylor instability |
| title_short | Centrifugally forced Rayleigh-Taylor instability |
| title_sort | centrifugally forced rayleigh-taylor instability |
| url | https://eprints.nottingham.ac.uk/52611/ https://eprints.nottingham.ac.uk/52611/ https://eprints.nottingham.ac.uk/52611/ |