The onset of Taylor–Görtler vortices during impulsive spin-down to rest
The onset of hydrodynamical instability induced by impulsive spin-down to rest in a cylinder containing a Newtonian fluid is analyzed by using the propagation theory. The primary transient swirl flow is laminar but for an initially high rotating speed secondary motion sets in at a certain time. It i...
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Published in | Chemical engineering science Vol. 61; no. 19; pp. 6478 - 6485 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Oxford
Elsevier Ltd
01.10.2006
Elsevier |
Subjects | |
Online Access | Get full text |
ISSN | 0009-2509 1873-4405 |
DOI | 10.1016/j.ces.2006.06.019 |
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Summary: | The onset of hydrodynamical instability induced by impulsive spin-down to rest in a cylinder containing a Newtonian fluid is analyzed by using the propagation theory. The primary transient swirl flow is laminar but for an initially high rotating speed secondary motion sets in at a certain time. It is found here that the critical Reynolds number
Re
c
=
320
, below which the flow is unconditionally stable. For
Re
>
Re
c
the dimensionless critical time
τ
c
to mark the onset of a fastest growing instability is presented as a function of the Reynolds number
Re. Available experimental data and also predictions show that deviation of the velocity profiles from their primary ones occurs starting from a certain time
τ
≈
4
τ
c
. This means that secondary motion is detected experimentally at this characteristic time. It seems that during
τ
c
⩽
τ
⩽
4
τ
c
secondary motion is relatively very weak. |
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Bibliography: | ObjectType-Article-2 SourceType-Scholarly Journals-1 ObjectType-Feature-1 content type line 23 |
ISSN: | 0009-2509 1873-4405 |
DOI: | 10.1016/j.ces.2006.06.019 |