scholarly journals Transition to turbulence in Taylor-Couette ferrofluidic flow

2015 ◽  
Vol 5 (1) ◽  
Author(s):  
Sebastian Altmeyer ◽  
Younghae Do ◽  
Ying-Cheng Lai
2020 ◽  
Vol 892 ◽  
Author(s):  
Christopher J. Crowley ◽  
Michael C. Krygier ◽  
Daniel Borrero-Echeverry ◽  
Roman O. Grigoriev ◽  
Michael F. Schatz


2014 ◽  
Vol 742 ◽  
pp. 254-290 ◽  
Author(s):  
Simon Maretzke ◽  
Björn Hof ◽  
Marc Avila

AbstractNon-normal transient growth of disturbances is considered as an essential prerequisite for subcritical transition in shear flows, i.e. transition to turbulence despite linear stability of the laminar flow. In this work we present numerical and analytical computations of linear transient growth covering all linearly stable regimes of Taylor–Couette flow. Our numerical experiments reveal comparable energy amplifications in the different regimes. For high shear Reynolds numbers$\mathit{Re}$, the optimal transient energy growth always follows a$\mathit{Re}^{2/3}$scaling, which allows for large amplifications even in regimes where the presence of turbulence remains debated. In co-rotating Rayleigh-stable flows, the optimal perturbations become increasingly columnar in their structure, as the optimal axial wavenumber goes to zero. In this limit of axially invariant perturbations, we show that linear stability and transient growth are independent of the cylinder rotation ratio and we derive a universal$\mathit{Re}^{2/3}$scaling of optimal energy growth using Wentzel–Kramers–Brillouin theory. Based on this, a semi-empirical formula for the estimation of linear transient growth valid in all regimes is obtained.


2016 ◽  
Vol 2016 (0) ◽  
pp. 0508
Author(s):  
Kouhei TAKASE ◽  
Yoshihiko OISHI ◽  
Hideki KAWAI ◽  
Hiroshige KIKURA ◽  
Hideki MURAKAWA

1996 ◽  
Author(s):  
M. Biage ◽  
Scott Harris ◽  
Scott Harris ◽  
W. Lempert ◽  
A. Smits

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