Abstract

This paper reviews recent advances and current debates in modeling the solar cycle as a hydromagnetic dynamo process. Emphasis is placed on (relatively) simple dynamo models that are nonetheless detailed enough to be comparable to solar cycle observations. After a brief overview of the dynamo problem and of key observational constraints, we begin by reviewing the various magnetic field regeneration mechanisms that have been proposed in the solar context. We move on to a presentation and critical discussion of extant solar cycle models based on these mechanisms. We then turn to the origin of fluctuations in these models, including amplitude and parity modulation, chaotic behavior, and intermittency. The paper concludes with a discussion of our current state of ignorance regarding various key questions, the most pressing perhaps being the identification of the physical mechanism(s) responsible for the generation of the Sun’s poloidal magnetic field component.

Highlights

  • This paper reviews recent advances and current debates in modeling the solar cycle as a hydromagnetic dynamo process

  • In the solar cycle context, the dynamo problem is reformulated towards identifying the circumstances under which the flow fields observed and/or inferred in the Sun can sustain the cyclic regeneration of the magnetic field associated with the observed solar cycle

  • The introduction of diffusivity quenching reduces the diffusivity in the shear region, “naturally” turning the model into a bona fide interface dynamo, supporting once again oscillatory solutions in the form of dynamo waves travelling in the “latitudinal” x-direction. This basic model was later generalized by various authors (Tobias, 1997; Phillips et al, 2002) to include the nonlinear backreaction of the dynamo-generated magnetic field on the differential rotation; further discussion of such nonlinear models is deferred to Section 5.3.1

Read more

Summary

Scope of review

The cyclic regeneration of the Sun’s large-scale magnetic field is at the root of all phenomena collectively known as “solar activity”. A near-consensus exists to the effect that this magnetic cycle is to be ascribed to the inductive action of fluid motions pervading the solar interior. At this writing nothing resembling consensus exists regarding the detailed nature and relative importance of various possible inductive flow contributions. To review “dynamo models of the solar cycle”, is daunting. This review focuses on the cyclic regeneration of the large-scale solar magnetic field through the inductive action of fluid flows, as described by various approximations and simplifications of the partial differential equations of magnetohydrodynamics. The focus is on models of the solar cycle, i.e., constructs seeking primarily to describe the observed spatio-temporal variations of the Sun’s large-scale magnetic field

What is a “model”?
A brief historical survey
Sunspots and the butterfly diagram
Organization of review
Magnetized fluids and the MHD induction equation
The dynamo problem
Kinematic models
Axisymmetric formulation
Boundary conditions and parity
Mechanisms of Magnetic Field Generation
Poloidal to toroidal
Toroidal to poloidal
Turbulence and mean-field electrodynamics
Hydrodynamical shear instabilities
MHD instabilities
The Babcock–Leighton mechanism
A Selection of Representative Models
Model ingredients
Calculating the α-effect and turbulent diffusivity
The αΩ dynamo equations
Eigenvalue problems and initial value problems
Dynamo waves
Representative results
Critical assessment
Strong α-quenching and the saturation problem
Mean-field models including meridional circulation
Models based on shear instabilities
From instability to α-effect
Representative solutions
Models based on buoyant instabilities of sheared magnetic layers
Babcock–Leighton models
Formulation of a poloidal source term
Numerical simulations of solar dynamo action
The observational evidence
Fossil fields and the 22-yr cycle
Backreaction on large-scale flows
Dynamical α-quenching
Time-delay dynamics
Time-delays in Babcock–Leighton models
Reduction to an iterative map
Stochastic forcing
The Maunder Minimum and intermittency
Intermittency from stochastic noise
Intermittency from nonlinearities
Intermittency from threshold effects
Intermittency from time delays
What is the primary poloidal field regeneration mechanism?
What limits the amplitude of the solar magnetic field?
Flux tubes versus diffuse fields
How constraining is the sunspot butterfly diagram?
Is meridional circulation crucial?
Is the mean solar magnetic field really axisymmetric?
Findings
What causes Maunder-type Grand Minima?
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call