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 inChemical engineering science Vol. 61; no. 19; pp. 6478 - 6485
Main Authors Kim, Min Chan, Kyun Choi, Chang
Format Journal Article
LanguageEnglish
Published Oxford Elsevier Ltd 01.10.2006
Elsevier
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ISSN0009-2509
1873-4405
DOI10.1016/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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ISSN:0009-2509
1873-4405
DOI:10.1016/j.ces.2006.06.019