2013
DOI: 10.1016/j.physleta.2013.06.007
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Feasible homopolar dynamo with sliding liquid-metal contacts

Abstract: We present a feasible homopolar dynamo design consisting of a flat, multi-arm spiral coil, which is placed above a fast-spinning metal ring and connected to the latter by sliding liquid-metal electrical contacts. Using a simple, analytically solvable axisymmetric model, we determine the optimal design of such a setup. For small contact resistance, the lowest magnetic Reynolds number, Rm ≈ 34.6, at which the dynamo can work, is attained at the optimal ratio of the outer and inner radii of the rings R i /R o ≈ 0… Show more

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Cited by 8 publications
(36 citation statements)
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“…However, provided the layers are thin enough, an anisotropic conductivity model is relevant to design such a dynamo experiment. Another dynamo experiment design with spiraling wires has been studied [16].…”
Section: Discussionmentioning
confidence: 99%
“…However, provided the layers are thin enough, an anisotropic conductivity model is relevant to design such a dynamo experiment. Another dynamo experiment design with spiraling wires has been studied [16].…”
Section: Discussionmentioning
confidence: 99%
“…The design consists of a flat multi-arm spiral coil placed above a fast-spinning copper disc and connected to the latter by sliding liquid-metal electrical contacts. The theoretical results obtained in [5] show a minimum magnetic Reynolds number of 40, at which the dynamo is self-excited. This can be achieved by using a copper disc of 60 cm in diameter which rotates with the frequency of 10 Hz.…”
Section: Introductionmentioning
confidence: 90%
“…, the voltage induced across the disc rotating with angular velocity Ω can be written according to the theoretical model of Priede et al [5] as…”
Section: Interpretation Of Experimental Datamentioning
confidence: 99%
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“…Model dynamos have been extensively investigated in the past as an aid to understanding the generation of magnetic fields and their reversals in astrophysical bodies. In 1979, Moffatt pointed out that the conventional treatment of the simplest such model [Moffatt, 1979], the self-exciting Bullard dynamo [Knobloch, 1981;Hide et al, 1996;Moroz et al, 1998;Priede & Avalos-Zúñiga, 2013], was not self-consistent because it neglected the currents associated with the radial diffusion of the magnetic field, and so introduced a segmented disc dynamo in which this effect could be included in a simple way. This dynamo is described by the following system of nondimensionalized ordinary differential equations:…”
Section: Description Of the Self-exciting Homopolar Disc Dynamo And Rmentioning
confidence: 99%