E.J. Spence
University of Wisconsin-Madison
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Featured researches published by E.J. Spence.
Physical Review Letters | 2006
E.J. Spence; M. D. Nornberg; C. M. Jacobson; R. D. Kendrick; Cary Forest
An axisymmetric magnetic field is applied to a spherical, turbulent flow of liquid sodium. An induced magnetic dipole moment is measured which cannot be generated by the interaction of the axisymmetric mean flow with the applied field, indicating the presence of a turbulent electromotive force. It is shown that the induced dipole moment should vanish for any axisymmetric laminar flow. Also observed is the production of toroidal magnetic field from applied poloidal magnetic field (the omega effect). Its potential role in the production of the induced dipole is discussed.
Physical Review E | 2007
R. A. Bayliss; Cary Forest; M. D. Nornberg; E.J. Spence; P. W. Terry
The role of turbulence in current generation and self-excitation of magnetic fields has been studied in the geometry of a mechanically driven, spherical dynamo experiment, using a three-dimensional numerical computation. A simple impeller model drives a flow that can generate a growing magnetic field, depending on the magnetic Reynolds number Rm=micro0sigmaVa and the fluid Reynolds number Re=Vanu of the flow. For Re<420, the flow is laminar and the dynamo transition is governed by a threshold of Rmcrit=100, above which a growing magnetic eigenmode is observed that is primarily a dipole field transverse to the axis of symmetry of the flow. In saturation, the Lorentz force slows the flow such that the magnetic eigenmode becomes marginally stable. For Re>420 and Rm approximately 100 the flow becomes turbulent and the dynamo eigenmode is suppressed. The mechanism of suppression is a combination of a time varying large-scale field and the presence of fluctuation driven currents (such as those predicted by the mean-field theory), which effectively enhance the magnetic diffusivity. For higher Rm, a dynamo reappears; however, the structure of the magnetic field is often different from the laminar dynamo. It is dominated by a dipolar magnetic field aligned with the axis of symmetry of the mean-flow, which is apparently generated by fluctuation-driven currents. The magnitude and structure of the fluctuation-driven currents have been studied by applying a weak, axisymmetric seed magnetic field to laminar and turbulent flows. An Ohms law analysis of the axisymmetric currents allows the fluctuation-driven currents to be identified. The magnetic fields generated by the fluctuations are significant: a dipole moment aligned with the symmetry axis of the mean-flow is generated similar to those observed in the experiment, and both toroidal and poloidal flux expulsion are observed.
Physical Review Letters | 2006
M. D. Nornberg; E.J. Spence; R. D. Kendrick; C. M. Jacobson; Cary Forest
The magnetic field measured in the Madison dynamo experiment shows intermittent periods of growth when an axial magnetic field is applied. The geometry of the intermittent field is consistent with the fastest-growing magnetic eigenmode predicted by kinematic dynamo theory using a laminar model of the mean flow. Though the eigenmodes of the mean flow are decaying, it is postulated that turbulent fluctuations of the velocity field change the flow geometry such that the eigenmode growth rate is temporarily positive. Therefore, it is expected that a characteristic of the onset of a turbulent dynamo is magnetic intermittency.
The Astrophysical Journal | 2009
E.J. Spence; K. Reuter; Cary Forest
We propose a plasma experiment to be used to investigate fundamental properties of astrophysical dynamos. The highly conducting, fast-flowing plasma will allow experimenters to explore systems with magnetic Reynolds numbers an order of magnitude larger than those accessible with liquid-metal experiments. The plasma is confined using a ring-cusp strategy and subject to a toroidal differentially rotating outer boundary condition. As proof of principle, we present magnetohydrodynamic simulations of the proposed experiment. When a von Karman-type boundary condition is specified, and the magnetic Reynolds number is large enough, dynamo action is observed. At different values of the magnetic Prandtl and Reynolds numbers the simulations demonstrate either laminar or turbulent dynamo action.
Physics of Plasmas | 2006
M. D. Nornberg; E.J. Spence; R. D. Kendrick; C. M. Jacobson; Cary Forest
Initial results from the Madison Dynamo Experiment provide details of the inductive response of a turbulent flow of liquid sodium to an applied magnetic field. The magnetic field structure is reconstructed from both internal and external measurements. A mean toroidal magnetic field is induced by the flow when an axial field is applied, thereby demonstrating the omega effect. Poloidal magnetic flux is expelled from the fluid by the poloidal flow. Small-scale magnetic field structures are generated by turbulence in the flow. The resulting magnetic power spectrum exhibits a power-law scaling consistent with the equipartition of the magnetic field with a turbulent velocity field. The magnetic power spectrum has an apparent knee at the resistive dissipation scale. Large-scale eddies in the flow cause significant changes to the instantaneous flow profile resulting in intermittent bursts of nonaxisymmetric magnetic fields, demonstrating that the transition to a dynamo is not smooth for a turbulent flow.
Archive | 2001
R. O’Connell; R. D. Kendrick; M. D. Nornberg; E.J. Spence; Adam Bayliss; Cary Forest
The cause of spontaneous generation of magnetic fields in conducting bodies (such as plasmas) is a longstanding, major problem in plasma astrophysics, geophysics, and laboratory plasmas. It is observed that magnetic fields exist in the Earth, Sun and other stars (and perhaps in galaxies), that cannot be explained as surviving primordial fields, and generally believed that such magnetic fields are generated by plasma flow (or flow of liquid metal for the Earth). The question of how magnetic fields are generated by unconstrained flows of conducting fluids and plasma is referred to as the“dynamo” problem; theoretical research into dynamo mechanisms has been actively pursued for several decades. However, until quite recently our probing of the dynamo problem has been limited to analytic calculations, numerical modelling and observational studies; experimental validation (the critical test for any theory) of aspects of the theory and experimental studies of laboratory dynamos have been scarce.
Physical Review Letters | 2007
E.J. Spence; M. D. Nornberg; C. M. Jacobson; C. A. Parada; N. Z. Taylor; R. D. Kendrick; Cary Forest
Archive | 2002
Cary B. Forest; R. Adam B. Bayliss; R. D. Kendrick; M. D. Nornberg; Robert W. O'Connell; E.J. Spence
Physical Review Letters | 2011
E. J. Kaplan; M.M. Clark; M. D. Nornberg; K. Rahbarnia; A.M. Rasmus; N. Z. Taylor; Cary B Forest; E.J. Spence
Bulletin of the American Physical Society | 2005
R. D. Kendrick; Cary B Forest; C.M. Jacobson; Nornberg; C.A. Parada; E.J. Spence