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相关论文: Theories of the solar cycle : a critical view

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The most promising model for explaining the origin of solar magnetism is the flux transport dynamo model, in which the toroidal field is produced by differential rotation in the tachocline, the poloidal field is produced by the…

太阳与恒星天体物理 · 物理学 2015-05-19 Arnab Rai Choudhuri

Sunspots and the plethora of other phenomena occuring in the course of the 11-year cycle of solar activity are a consequence of the emergence of magnetic flux at the solar surface. The observed orientations of bipolar sunspot groups imply…

太阳与恒星天体物理 · 物理学 2015-06-24 Robert Cameron , Manfred Schüssler

The magnetic activity of the Sun, as manifested in the sunspot cycle, originates deep within its convection zone through a dynamo mechanism which involves non-trivial interactions between the plasma and magnetic field in the solar interior.…

太阳与恒星天体物理 · 物理学 2015-05-13 Dibyendu Nandy

Many stars exhibit strong magnetic fields, some of which are thought to be of primordial origin and others a sign of magnetic dynamo processes. We briefly review the results of observational studies of solar-type stars seeking to evaluate…

天体物理学 · 物理学 2007-05-23 Allan Sacha Brun

The phenomenon of solar "torsional oscillations" (TO) represents migratory zonal flows associated with the solar cycle. These flows are observed on the solar surface and, according to helioseismology, extend through the convection zone. We…

太阳与恒星天体物理 · 物理学 2016-08-31 G. Guerrero , P. K. Smolarkiewicz , E. M. de Gouveia Dal Pino , A. G. Kosovichev , N. N. Mansour

A comprehensive understanding of the solar magnetic cycle requires detailed modeling of the solar interior including the maintenance and variation of large scale flows (differential rotation and meridional flow), the solar dynamo and the…

太阳与恒星天体物理 · 物理学 2010-10-29 M. Rempel

The solar tachocline is an internal region of the Sun possessing strong radial and latitudinal shears straddling the base of the convective envelope. Based on helioseismic inversions, the tachocline is known to be thin (less than 5\% of the…

太阳与恒星天体物理 · 物理学 2023-11-22 Antoine Strugarek , Bernadett Belucz , Allan Sacha Brun , Mausumi Dikpati , Gustavo Guerrero

Gough & McIntyre have suggested that the dynamics of the solar tachocline are dominated by the advection-diffusion balance between the differential rotation, a large-scale primordial field and baroclinicly driven meridional motions. This…

天体物理学 · 物理学 2009-11-07 P. Garaud

The solar cycle is a complex phenomenon. To comprehensively understand it, we have to study various tracers. The most important component of this complex is the solar dynamo, which is understood as self-excitation of the solar magnetic…

太阳与恒星天体物理 · 物理学 2025-01-10 V. N. Obridko , A. S. Shibalova , D. D. Sokoloff

The solar tachocline, located at the interface between the latitude-dependent rotation of the convection zone and the rigid radiative interior, presents high gradients of angular velocity which are of particular interest for the models of…

天体物理学 · 物理学 2013-08-01 T. Corbard , S. J. Jiménez-Reyes , S. Tomczyk , M. Dikpati , P. Gilman

The tachocline is believed to be the region where the solar dynamo operates. With over a solar cycle's worth of data available from the MDI and GONG instruments, we are in a position to investigate not merely the average structure of the…

太阳与恒星天体物理 · 物理学 2015-05-28 H. M. Antia , Sarbani Basu

The details of the dynamo process that is responsible for driving the solar magnetic activity cycle are still not fully understood. In particular, whilst differential rotation provides a plausible mechanism for the regeneration of the…

太阳与恒星天体物理 · 物理学 2024-10-14 Craig D. Duguid , Paul J. Bushby , Toby S. Wood

The toroidal magnetic field is assumed to be generated in the tachocline in most Babcock-Leighton (BL)-type solar dynamo models, in which the poloidal field is produced by the emergence and subsequent dispersal of sunspot groups. However,…

太阳与恒星天体物理 · 物理学 2022-05-11 Zebin Zhang , Jie Jiang

The exact location of the solar dynamo remains uncertain--whether it operates primarily in the near-surface shear layer, throughout the entire convection zone, or near the tachocline, a region of sharp transition in the solar rotation,…

太阳与恒星天体物理 · 物理学 2026-01-07 Krishnendu Mandal , Alexander G. Kosovichev

The leading theoretical paradigm for the Sun's magnetic cycle is an $\alpha\omega$-dynamo process, in which a combination of differential rotation and turbulent, helical flows produces a large-scale magnetic field that reverses every 11…

太阳与恒星天体物理 · 物理学 2023-01-16 Craig D. Duguid , Paul J. Bushby , Toby S. Wood

Recent analysis of the helioseismic observations indicate that the previously observed surface torsional oscillations extend significantly downwards into the solar convection zone. In an attempt to understand these oscillations, we study…

天体物理学 · 物理学 2007-05-23 Eurico Covas , Reza Tavakol , David Moss , Andrew Tworkowski

Two fundamental properties of stellar magnetic fields have been determined by observations for solar-like stars with different Rossby numbers (Ro), namely, the magnetic field strength and the magnetic cycle period. The field strength…

太阳与恒星天体物理 · 物理学 2019-07-24 G. Guerrero , B. Zaire , P. K. Smolarkiewicz , E. M. de Gouveia Dal Pino , A. G. Kosovichev , N. N. Mansour

We present a nonlinear mean-field model of the solar interior dynamics and dynamo, which reproduces the observed cyclic variations of the global magnetic field of the Sun, as well as the differential rotation and meridional circulation.…

太阳与恒星天体物理 · 物理学 2020-01-08 V. V. Pipin , A. G. Kosovichev

Rotational shear layers at the boundary between radiative and convective zones, tachoclines, play a key role in the process of magnetic field generation in solar-like stars. We present two sets of global simulations of rotating turbulent…

太阳与恒星天体物理 · 物理学 2016-03-08 G. Guerrero , P. K. Smolarkiewicz , E. M. de Gouveia Dal Pino , A. G. Kosovichev , N. N. Mansour

The Sun's magnetic dynamo cycle features a distinct pattern: a propagating region of sunspot emergence appears around 30 degrees latitude and vanishes near the equator every 11 years. Moreover, longitudinal flows called "torsional…

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