×
Well done. You've clicked the tower. This would actually achieve something if you had logged in first. Use the key for that. The name takes you home. This is where all the applicables sit. And you can't apply any changes to my site unless you are logged in.

Our policy is best summarized as "we don't care about _you_, we care about _them_", no emails, so no forgetting your password. You have no rights. It's like you don't even exist. If you publish material, I reserve the right to remove it, or use it myself.

Don't impersonate. Don't name someone involuntarily. You can lose everything if you cross the line, and no, I won't cancel your automatic payments first, so you'll have to do it the hard way. See how serious this sounds? That's how serious you're meant to take these.

×
Register


Required. 150 characters or fewer. Letters, digits and @/./+/-/_ only.
  • Your password can’t be too similar to your other personal information.
  • Your password must contain at least 8 characters.
  • Your password can’t be a commonly used password.
  • Your password can’t be entirely numeric.

Enter the same password as before, for verification.
Login

Grow A Dic
Define A Word
Make Space
Set Task
Mark Post
Apply Votestyle
Create Votes
(From: saved spaces)
Exclude Votes
Apply Dic
Exclude Dic

Click here to flash read.

Our theoretical and numerical analysis have suggested that for low-mass main
sequences stars (of the spectral classes from M5 to G0) rotating much faster
than the Sun, the generated large-scale magnetic field is caused by the
mean-field $\alpha^2\Omega$ dynamo, whereby the $\alpha^2$ dynamo is modified
by a weak differential rotation. Even for a weak differential rotation, the
behaviour of the magnetic activity is changed drastically from aperiodic regime
to nonlinear oscillations and appearance of a chaotic behaviour with increase
of the differential rotation. Periods of the magnetic cycles decrease with
increase of the differential rotation, and they vary from tens to thousand
years. This long-term behaviour of the magnetic cycles may be related to the
characteristic time of the evolution of the magnetic helicity density of the
small-scale field. The performed analysis is based on the mean-field numerical
simulations of the $\alpha^2\Omega$ and $\alpha^2$ dynamos and a developed
nonlinear theory of $\alpha^2$ dynamo.

Click here to read this post out
ID: 377830; Unique Viewers: 0
Unique Voters: 0
Total Votes: 0
Votes:
Latest Change: Sept. 6, 2023, 7:31 a.m. Changes:
Dictionaries:
Words:
Spaces:
Views: 10
CC:
No creative common's license
Comments: