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Stellar Dynamos

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Solar and Stellar Dynamos

Part of the book series: Saas-Fee Advanced Courses ((SAASFEE,volume 39))

Abstract

This chapter steps finally away from the sun and towards the stars, the idea being to apply the physical insight gained so far to see how much of stellar magnetism can be understood in terms of dynamo action. Dynamo action in the convective core of massive main-sequence stars is first considered and shown viable. For intermediate-mass main-sequence stars the fossil field hypothesis will carry the day, although possible dynamo alternatives are also briefly discussed. The extension of the solar dynamo models investigated in Chap. 3 to other solar-type stars will first take us through an important detour in first having to understand rotational evolution in response to angular momentum loss in a magnetized wind. Dynamo action in fully convective stars comes next, and the chapter closes with an overview of the situation for pre- and post-main-sequence stars and compact objects, leading finally to the magnetic fields of galaxies and beyond.

ELWOOD: It’s 106 miles to Chicago, we’ve got a full tank of gas, half a pack of cigarettes, it’s dark and we’re wearing sunglasses. JAKE: Hit it!

Dan Ackroyd and John Belushi

The Blues Brothers (1980)

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Notes

  1. 1.

    The content of this section is based on the paper by Charbonneau and MacGregor (2001) given in the bibliography.

  2. 2.

    The \(\alpha ^2\) form of the mean-field dynamo equations also admits growing solutions that are non-axisymmetric even though the \(\alpha \)-effect profile exhibits axisymmetry with respect to the rotation axis. Growth rates for non-axisymmetric modes are often comparable to those of their axisymmetric counterparts. Motivated largely by the challenge posed by planetary magnetic fields, \(\alpha ^2\) models can and have been constructed where non-axisymmetric modes are the fastest growing, and dominate in the moderately supercritical nonlinear regime. For complex enough spatial profiles of \(\alpha \), i.e., including multiple sign changes in each hemisphere, it is also possible to produce \(\alpha ^2\) dynamo solutions undergoing cyclic polarity reversals.

  3. 3.

    The content of this section is based primarily on the paper by Brun et al. (2005) given in the bibliography.

  4. 4.

    Note however that the above relation was calibrated in a relatively narrow range of parameters: \(2\le u_0\le 30\,\)m s\(^{-1}\), \(0.03\le s_0\le 1\,\)m s\(^{-1}\), \(2\times 10^6\le \eta _0\le 5\times 10^7\,\)m\(^2\) s\(^{-1}\), and is only expected to hold in the so-called advection-dominated regime; see the paper by Dikpati & Charbonneau (1999) cited in the bibliography of Chap. 3.

  5. 5.

    The content of this section is based primarily on the paper by Dobler et al. (2006).

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Charbonneau, P. (2013). Stellar Dynamos. In: Steiner, O. (eds) Solar and Stellar Dynamos. Saas-Fee Advanced Courses, vol 39. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-32093-4_5

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  • DOI: https://doi.org/10.1007/978-3-642-32093-4_5

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