Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical Dynamos

The relative importance of the helicity and cross-helicity electromotive dynamo effects for self-sustained magnetic field generation by chaotic thermal convection in rotating spherical shells is investigated as a function of shell thickness. Two distinct branches of dynamo solutions are found to coe...

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Main Authors: Luis Silva, Parag Gupta, David MacTaggart, Radostin D. Simitev
Format: Article
Language:English
Published: MDPI AG 2020-12-01
Series:Fluids
Subjects:
Online Access:https://www.mdpi.com/2311-5521/5/4/245
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spelling doaj-5542d43384024f1e8b8e1c4a243b0c572020-12-17T00:01:21ZengMDPI AGFluids2311-55212020-12-01524524510.3390/fluids5040245Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical DynamosLuis Silva0Parag Gupta1David MacTaggart2Radostin D. Simitev3School of Mathematics and Statistics, University of Glasgow, Glasgow G12 8QQ, UKSchool of Mathematics and Statistics, University of Glasgow, Glasgow G12 8QQ, UKSchool of Mathematics and Statistics, University of Glasgow, Glasgow G12 8QQ, UKSchool of Mathematics and Statistics, University of Glasgow, Glasgow G12 8QQ, UKThe relative importance of the helicity and cross-helicity electromotive dynamo effects for self-sustained magnetic field generation by chaotic thermal convection in rotating spherical shells is investigated as a function of shell thickness. Two distinct branches of dynamo solutions are found to coexist in direct numerical simulations for shell aspect ratios between 0.25 and 0.6—a mean-field dipolar regime and a fluctuating dipolar regime. The properties characterising the coexisting dynamo attractors are compared and contrasted, including differences in temporal behaviour and spatial structures of both magnetic fields and rotating thermal convection. The helicity <inline-formula><math display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>-effect and the cross-helicity <inline-formula><math display="inline"><semantics><mi>γ</mi></semantics></math></inline-formula>-effect are found to be comparable in intensity within the fluctuating dipolar dynamo regime, where their ratio does not vary significantly with the shell thickness. In contrast, within the mean-field dipolar dynamo regime the helicity <inline-formula><math display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>-effect dominates by approximately two orders of magnitude and becomes stronger with decreasing shell thickness.https://www.mdpi.com/2311-5521/5/4/245rotating thermal convectionconvection-driven dynamosnumerical simulationsbistabilitymean-field magnetohydrodynamicsspherical shells
collection DOAJ
language English
format Article
sources DOAJ
author Luis Silva
Parag Gupta
David MacTaggart
Radostin D. Simitev
spellingShingle Luis Silva
Parag Gupta
David MacTaggart
Radostin D. Simitev
Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical Dynamos
Fluids
rotating thermal convection
convection-driven dynamos
numerical simulations
bistability
mean-field magnetohydrodynamics
spherical shells
author_facet Luis Silva
Parag Gupta
David MacTaggart
Radostin D. Simitev
author_sort Luis Silva
title Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical Dynamos
title_short Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical Dynamos
title_full Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical Dynamos
title_fullStr Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical Dynamos
title_full_unstemmed Effects of Shell Thickness on Cross-Helicity Generation in Convection-Driven Spherical Dynamos
title_sort effects of shell thickness on cross-helicity generation in convection-driven spherical dynamos
publisher MDPI AG
series Fluids
issn 2311-5521
publishDate 2020-12-01
description The relative importance of the helicity and cross-helicity electromotive dynamo effects for self-sustained magnetic field generation by chaotic thermal convection in rotating spherical shells is investigated as a function of shell thickness. Two distinct branches of dynamo solutions are found to coexist in direct numerical simulations for shell aspect ratios between 0.25 and 0.6—a mean-field dipolar regime and a fluctuating dipolar regime. The properties characterising the coexisting dynamo attractors are compared and contrasted, including differences in temporal behaviour and spatial structures of both magnetic fields and rotating thermal convection. The helicity <inline-formula><math display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>-effect and the cross-helicity <inline-formula><math display="inline"><semantics><mi>γ</mi></semantics></math></inline-formula>-effect are found to be comparable in intensity within the fluctuating dipolar dynamo regime, where their ratio does not vary significantly with the shell thickness. In contrast, within the mean-field dipolar dynamo regime the helicity <inline-formula><math display="inline"><semantics><mi>α</mi></semantics></math></inline-formula>-effect dominates by approximately two orders of magnitude and becomes stronger with decreasing shell thickness.
topic rotating thermal convection
convection-driven dynamos
numerical simulations
bistability
mean-field magnetohydrodynamics
spherical shells
url https://www.mdpi.com/2311-5521/5/4/245
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