The Magnetorotational Instability (MRI)

2013 ◽  
pp. 185-246
2009 ◽  
Vol 45 (2) ◽  
pp. 135-144 ◽  
Author(s):  
F. Stefani ◽  
G. Gerbeth ◽  
Th. Gundrum ◽  
J. Szklarski ◽  
G. Rüdiger ◽  
...  

2007 ◽  
Vol 659 (2) ◽  
pp. 1496-1504 ◽  
Author(s):  
M. Furukawa ◽  
Z. Yoshida ◽  
M. Hirota ◽  
V. Krishan

2018 ◽  
Vol 10 (6) ◽  
pp. 721-729
Author(s):  
V. M. Chechetkin ◽  
K. R. Sychugov ◽  
A. Yu. Lugovsky ◽  
A. N. Pastuhov

2016 ◽  
Vol 461 (2) ◽  
pp. 1614-1620 ◽  
Author(s):  
Quentin Kral ◽  
Henrik Latter

2008 ◽  
Vol 487 (1) ◽  
pp. 1-5 ◽  
Author(s):  
G. Bodo ◽  
A. Mignone ◽  
F. Cattaneo ◽  
P. Rossi ◽  
A. Ferrari

2015 ◽  
Vol 81 (4) ◽  
Author(s):  
K. Flanagan ◽  
M. Clark ◽  
C. Collins ◽  
C. M. Cooper ◽  
I. V. Khalzov ◽  
...  

Many astrophysical disks, such as protoplanetary disks, are in a regime where non-ideal, plasma-specific magnetohydrodynamic (MHD) effects can significantly influence the behaviour of the magnetorotational instability (MRI). The possibility of studying these effects in the plasma Couette experiment (PCX) is discussed. An incompressible, dissipative global stability analysis is developed to include plasma-specific two-fluid effects and neutral collisions, which are inherently absent in analyses of Taylor–Couette flows (TCFs) in liquid metal experiments. It is shown that with boundary driven flows, a ion-neutral collision drag body force significantly affects the azimuthal velocity profile, thus limiting the flows to regime where the MRI is not present. Electrically driven flow (EDF) is proposed as an alternative body force flow drive in which the MRI can destabilize at more easily achievable plasma parameters. Scenarios for reaching MRI relevant parameter space and necessary hardware upgrades are described.


2018 ◽  
Vol 113 (1-2) ◽  
pp. 51-70 ◽  
Author(s):  
F. Stefani ◽  
A. Gailitis ◽  
G. Gerbeth ◽  
A. Giesecke ◽  
Th. Gundrum ◽  
...  

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