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The Remarkable Rotational Braking of G5 Giants

Published online by Cambridge University Press:  04 August 2017

David F. Gray*
Affiliation:
University of Western Ontario, London, Ontario, Canada

Abstract

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The strong rotational braking seen in the G5 III stage of evolution may be the key to understanding how stellar dynamos work.

We are all familiar with the leisurely spin-down seen in cool main-sequence stars like our Sun. The time scales here are ∼ 109 years and the accepted cause is the loss of high angular momentum mass in the form of stellar winds interacting with the stellar magnetic field. The magnetic field is believed to result from the interaction of envelope convection with the rotation of the star through a dynamo mechanism. Our understanding of how a dynamo actually operates, how that operation depends on the driving forces of rotation and convection, what kind of stochastic and secular time variations are to be expected, remains fragmentary even though many inventive minds have contributed. One reason for slow progress is simply that the Sun is almost the only example of a stellar dynamo we have had. But nature has given us another, much more powerful dynamo in the G5 giants, it just took us a little longer to discover it.

Type
V. Stellar Winds and Spindown in Late — Type Stars
Copyright
Copyright © Reidel 1983 

References

Endal, A.S. and Sofia, S.: 1979, Astrophys. J. 232, p. 531.Google Scholar
Fukuda, I.: 1981, preprint.Google Scholar
Gray, D.F.: 1981, Astrophys. J. 251, p. 155.Google Scholar
Gray, D.F.: 1982a, Astrophys. J. 261, Oct. 15 issue.Google Scholar
Gray, D.F.: 1982b, Astrophys. J. 262, Nov. 15 issue.Google Scholar