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UK MHD Meeting 2004 

Thursday 6th and Friday 7th May 2004

Nice - Cote D'Azur

Laboratory Cassiopée UMR6202 CNRS 
Observatory of the Cote d'Azur

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Dynamo Simulations Using a High Order Cartesian Magnetohydrodynamics Code

Graeme_Sarson ,   University of Newcastle

Most numerical simulations of the geodynamo are cast in spherical geometry, using a spherical harmonic
representation for lateral variations and an expansion in Chebyshev polynomials or discretisation in radius. A number
of research groups have produced time dependent, three dimensional, self-consistent solutions to the geodynamo
problem using this pseudospectral methodology. Computational limitations currently place a practical bound on the
parameter regime that can be explored in this context, with values appropriate for Earth out of reach by several orders
of magnitude. For the spherically pseudospectral codes, the absence of an efficient Legendre transform is a strong
factor contributing to this limitation. As a first step towards alternative computational methods for geodynamo
modelling, we have adapted an existing, efficiently parallelised magnetohydrodynamics (MHD) code, originally
developed for weakly compressible, turbulent astrophysical MHD problems. The Pencil Code
(www.nordita.dk/data/brandenb/pencil-code) is a Cartesian code that uses sixth-order finite differences, applied to
``pencils'' (i.e. array sections) in the x direction in a cache-efficient way. The domain is tiled in the y and z
directions, with the communication of boundary elements handled by Message Passing Interface (MPI). Time stepping is
via a third order Runge-Kutta method. The code's modular structure allows a flexible selection of various physical
processes and variables, making it easily adaptable for many types of MHD problems, including spherical dynamos. We
demonstrate dynamo action driven by thermal convection in a spherical shell of ideal gas, for comparison with Kageyama
et al. (Phys. Plasmas, 2, 1421-1431, 1995). More realistic modelling of terrestrial dynamos requires the implementation
of Boussinesq or anelastic approximations. We report on our progress in this direction, and initial attempts to
reproduce the geodynamo benchmark (Christensen et al., Phys. Earth Planet. Int., 128, 25-34, 2001) by this approach.

   

 
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