Solar Field Mapping and Dynamo Behavior

We discuss the importance of the Sun’s large-scale magnetic field to the Sun-Planetary environment. This paper narrows its focus down to the motion and evolution of the photospheric large-scale magnetic field which affects many environments throughout this region. For this purpose we utilize a newly...

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Main Author: Kenneth H. Schatten
Format: Article
Language:English
Published: Hindawi Limited 2012-01-01
Series:Advances in Astronomy
Online Access:http://dx.doi.org/10.1155/2012/923578
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spelling doaj-1d881cbfaefe489988e2ebe07a3031252020-11-24T21:09:06ZengHindawi LimitedAdvances in Astronomy1687-79691687-79772012-01-01201210.1155/2012/923578923578Solar Field Mapping and Dynamo BehaviorKenneth H. Schatten0Solar Physics, a.i. solutions, Inc., Suite 215, 10001 Derekwood Lane, Lanham, MD 20706, USAWe discuss the importance of the Sun’s large-scale magnetic field to the Sun-Planetary environment. This paper narrows its focus down to the motion and evolution of the photospheric large-scale magnetic field which affects many environments throughout this region. For this purpose we utilize a newly developed Netlogo cellular automata model. The domain of this algorithmic model is the Sun’s photosphere. Within this computational space are placed two types of entities or agents; one may refer to them as bluebirds and cardinals; the former carries outward magnetic flux and the latter carries out inward magnetic flux. One may simply call them blue and red agents. The agents provide a granularity with discrete changes not present in smooth MHD models; they undergo three processes: birth, motion, and death within the photospheric domain. We discuss these processes, as well as how we are able to develop a model that restricts its domain to the photosphere and allows the deeper layers to be considered only through boundary conditions. We show the model’s ability to mimic a number of photospheric magnetic phenomena: the solar cycle (11-year) oscillations, the Waldmeier effect, unipolar magnetic regions (e.g. sectors and coronal holes), Maunder minima, and the march/rush to the poles involving the geometry of magnetic field reversals. We also discuss why the Sun sometimes appears as a magnetic monopole, which of course requires no alteration of Maxwell’s equations.http://dx.doi.org/10.1155/2012/923578
collection DOAJ
language English
format Article
sources DOAJ
author Kenneth H. Schatten
spellingShingle Kenneth H. Schatten
Solar Field Mapping and Dynamo Behavior
Advances in Astronomy
author_facet Kenneth H. Schatten
author_sort Kenneth H. Schatten
title Solar Field Mapping and Dynamo Behavior
title_short Solar Field Mapping and Dynamo Behavior
title_full Solar Field Mapping and Dynamo Behavior
title_fullStr Solar Field Mapping and Dynamo Behavior
title_full_unstemmed Solar Field Mapping and Dynamo Behavior
title_sort solar field mapping and dynamo behavior
publisher Hindawi Limited
series Advances in Astronomy
issn 1687-7969
1687-7977
publishDate 2012-01-01
description We discuss the importance of the Sun’s large-scale magnetic field to the Sun-Planetary environment. This paper narrows its focus down to the motion and evolution of the photospheric large-scale magnetic field which affects many environments throughout this region. For this purpose we utilize a newly developed Netlogo cellular automata model. The domain of this algorithmic model is the Sun’s photosphere. Within this computational space are placed two types of entities or agents; one may refer to them as bluebirds and cardinals; the former carries outward magnetic flux and the latter carries out inward magnetic flux. One may simply call them blue and red agents. The agents provide a granularity with discrete changes not present in smooth MHD models; they undergo three processes: birth, motion, and death within the photospheric domain. We discuss these processes, as well as how we are able to develop a model that restricts its domain to the photosphere and allows the deeper layers to be considered only through boundary conditions. We show the model’s ability to mimic a number of photospheric magnetic phenomena: the solar cycle (11-year) oscillations, the Waldmeier effect, unipolar magnetic regions (e.g. sectors and coronal holes), Maunder minima, and the march/rush to the poles involving the geometry of magnetic field reversals. We also discuss why the Sun sometimes appears as a magnetic monopole, which of course requires no alteration of Maxwell’s equations.
url http://dx.doi.org/10.1155/2012/923578
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