Abstract

We present results from three-dimensional nonlinear hydrodynamic simulations of a precession driven flow in cylindrical geometry. The simulations are motivated by a dynamo experiment currently under development at Helmholtz-Zentrum Dresden-Rossendorf in which the possibility of generating a magnetohydrodynamic dynamo will be investigated in a cylinder filled with liquid sodium and simultaneously rotating around two axes. In this study, we focus on the emergence of non-axisymmetric time-dependent flow structures in terms of inertial waves which—in cylindrical geometry—form so-called Kelvin modes. For a precession ratio (Poincaré number) considered by us, the amplitude of the forced Kelvin mode reaches up to one fourth of the rotation velocity of the cylindrical container confirming that precession provides a rather efficient flow driving mechanism even at moderate values of Po. More relevant for dynamo action might be free Kelvin modes with higher azimuthal wave number. These free Kelvin modes are triggered by nonlinear interactions and may constitute a triadic resonance with the fundamental forced mode when the height of the container matches their axial wave lengths. Our simulations reveal triadic resonances at aspect ratios close to those predicted by the linear theory except around the primary resonance of the forced mode. In that regime we still identify various free Kelvin modes, however, all of them exhibit a retrograde drift around the symmetry axis of the cylinder and none of them can be assigned to a triadic resonance. The amplitudes of the free Kelvin modes always remain below the forced mode but may reach up to 6% of the of the container’s angular velocity. The properties of the free Kelvin modes, namely their amplitude and their frequency, will be used in future simulations of the magnetic induction equation to investigate their ability to provide for dynamo action.

Highlights

  • Instabilities and waves in rotating fluids are important in numerous technical applications

  • The flow is clearly dominated by a velocity mode with m = 1 and k = 1. This is the primary Kelvin mode driven by the precessional forcing

  • The simulations confirm that the energy that can be injected via precessional forcing is very sensitive to the aspect ratio of the cylindrical container

Read more

Summary

Introduction

Instabilities and waves in rotating fluids are important in numerous technical applications. In the model of Moffatt (1970), field and flow must decay in the long term because of the lack of energy sources required for a steady driving This problem can be overcome by more complex models in which, for example, the equatorial heat flux in the Earth’s outer core provides a persistent excitation mechanism for inertial waves with sufficient helicity for the generation of planetary magnetic fields (Davidson 2014). Other experiments revealed large scale structures like a system of intermittent, cyclonic vortices that may provide a strong source of helicity and be beneficial for a dynamo (Mouhali et al 2012), or free Kelvin modes with an azimuthal wave number m = 5 and m = 6 propagating around the symmetry axis of a weakly precessing cylinder (Lagrange et al 2008, Lagrange et al 2011). The results are used to further constrain the modes that may be observed in the water experiment at HZDR‡ and will be applied in future simulations of the magnetic induction equation in order to proof whether free Kelvin modes are suitable to drive a dynamo

Theoretical background
Numerical model
Pattern of the total flow
Kinetic energy
Spatial Structure of the Fourier modes
Radial dependence
Amplitudes and frequencies
Azimuthal shear flow
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call