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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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 |
work_keys_str_mv |
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