Lagrangian chaos and the fast kinematic dynamo problem

Author(s):  
Edward Ott
Keyword(s):  
2006 ◽  
Vol 334 (10) ◽  
pp. 593-598 ◽  
Author(s):  
Raphael Laguerre ◽  
Caroline Nore ◽  
Jacques Léorat ◽  
Jean-Luc Guermond
Keyword(s):  

2014 ◽  
Vol 109 (2) ◽  
pp. 159-167 ◽  
Author(s):  
Xing Wei
Keyword(s):  

2002 ◽  
Vol 397 (2) ◽  
pp. 393-399 ◽  
Author(s):  
V. Archontis ◽  
S. B. F. Dorch ◽  
Å. Nordlund

2004 ◽  
Vol 196 (1) ◽  
pp. 102-125 ◽  
Author(s):  
M. Xu ◽  
F. Stefani ◽  
G. Gerbeth

2010 ◽  
Vol 74 (2) ◽  
pp. 165-176 ◽  
Author(s):  
A. Pinter ◽  
B. Dubrulle ◽  
F. Daviaud

2009 ◽  
Vol 5 (S264) ◽  
pp. 33-38
Author(s):  
Hiromoto Shibahashi

AbstractThe brilliant outcome of some 30 years of helioseismology spreads over a wide range of topics. Some highlights relevant to the cause of the solar activity cycle are listed up. The rotation profile in the solar convective zone is discussed as an important source of the dynamo mechanism. The kinematic dynamo model is described in the linear approximation, and the condition for the solar type dynamo is derived. It is shown that comparison of this condition with the rotation profile determined from helioseismology is useful to identify the possible seats of the dynamo.


1984 ◽  
Vol 144 ◽  
pp. 1-11 ◽  
Author(s):  
Ya. B. Zel'Dovich ◽  
A. A. Ruzmaikin ◽  
S. A. Molchanov ◽  
D. D. Sokoloff

A magnetic field is shown to be asymptotically (t → ∞) decaying in a flow of finite conductivity with v = Cr, where C = Cζ(t) is a random matrix. The decay is exponential, and its rate does not depend on the conductivity. However, the magnetic energy increases exponentially owing to growth of the domain occupied by the field. The spatial distribution of the magnetic field is a set of thin ropes and (or) layers.


2013 ◽  
Vol 3 (3) ◽  
pp. 032003
Author(s):  
Benlong Wang ◽  
Hua Liu

1996 ◽  
Vol 17 (2) ◽  
pp. 215-218
Author(s):  
Graeme Sarson
Keyword(s):  

1972 ◽  
Vol 176 ◽  
pp. 235 ◽  
Author(s):  
I. Lerche

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