2009
DOI: 10.1088/0953-2048/22/12/125026
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Pulsed-field magnetization of drilled bulk high-temperature superconductors: flux front propagation in the volume and on the surface

Abstract: We present a method for characterizing the propagation of the magnetic flux in an artificially drilled bulk high-temperature superconductor (HTS) during a pulsed-field magnetization. As the magnetic pulse penetrates the cylindrical sample, the magnetic flux density is measured simultaneously in 16 holes by means of microcoils that are placed across the median plane, i.e. at an equal distance from the top and bottom surfaces, and close to the surface of the sample. We discuss the time evolution of the magnetic … Show more

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Cited by 8 publications
(7 citation statements)
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“…a useful inner diameter larger than 10 mm. Strictly speaking, shielding at higher field was reported in tiny holes or gaps in/between bulk superconductors [27], [37] (1-2 mm), but such small bores are clearly out of the scope of the present study.…”
Section: Shielding Properties At Various Temperaturesmentioning
confidence: 69%
“…a useful inner diameter larger than 10 mm. Strictly speaking, shielding at higher field was reported in tiny holes or gaps in/between bulk superconductors [27], [37] (1-2 mm), but such small bores are clearly out of the scope of the present study.…”
Section: Shielding Properties At Various Temperaturesmentioning
confidence: 69%
“…The expected increase for an infinitely thick ferromagnetic "disc" is likely to be bounded by the increase that would occur for a semi-infinite ferromagnet. Since the latter configuration is equivalent to doubling the height of the superconducting disc, we can roughly estimate the effect of the ferromagnet from the analytical formula giving the magnetic flux density along the axis of a fully magnetized superconducting cylinder (radius a, height L, critical current density J c ) [10,54,55] …”
Section: Influence Of the Disc Thicknessmentioning
confidence: 99%
“…Furthermore, this simple model assumes a field-independent critical current density. The corresponding parameter J c0 , estimated from a Hall probe mapping measurement [52], invariably contains a degree of uncertainty because of (i) the finite distance between the probe and the sample surface and (ii) the difference between the trapped flux distribution above the top surface and that in the central plane [53,54]. Unlike the analytical expression of H tr2 (equation ( 1)) which is weakly influenced by an uncertainty on J c0 (due to the '1/3' exponent), the precise J c0 value affects directly the transient self-heating behaviour.…”
Section: Temperature Distribution During Self-heating-experiments And...mentioning
confidence: 99%