1986
DOI: 10.1051/rphysap:01986002109056300
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Sur les champs magnétiques pulsés crowbar. I. Caractéristiques géométriques et électriques des bobines en cuivre

Abstract: 2014 Un champ pulsé est défini par le champ crête B0, l'énergie magnétique W et le rayon intérieur a1 des bobines. Nous proposons un ensemble de formules qui, pour chaque couple w = W/2,5 a31 B20 et 0393 = diamètre extérieur/longueur des bobines, donnent : l'« épaisseur » de chaque bobine, leur constante de temps, l'homogénéïté du champ magnétique, la température du bobinage à la fin d'une impulsion crowbar. Nous montrons, que pour chaque champ pulsé, c'est dans la bobine 0393 = 1,36, que les contraintes magné… Show more

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Cited by 15 publications
(8 citation statements)
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“…Keeping in mind that (i) a magnetic field stabilises the highest spin‐state of the molecule through the Zeeman effect, (ii) the spin crossover phenomenon is a dynamic process and (iii) it is possible to generate high pulsed magnetic fields21 (LNCMP/CNRS, Toulouse, France: 32 Tesla in 2000 and 60 Tesla currently), the idea of applying a pulsed magnetic field in the hysteresis loop was developed.…”
Section: Switching Of Spin States By External Perturbationsmentioning
confidence: 99%
“…Keeping in mind that (i) a magnetic field stabilises the highest spin‐state of the molecule through the Zeeman effect, (ii) the spin crossover phenomenon is a dynamic process and (iii) it is possible to generate high pulsed magnetic fields21 (LNCMP/CNRS, Toulouse, France: 32 Tesla in 2000 and 60 Tesla currently), the idea of applying a pulsed magnetic field in the hysteresis loop was developed.…”
Section: Switching Of Spin States By External Perturbationsmentioning
confidence: 99%
“…The pulsed field facility at LNCMP (Toulouse) [34] produces fields up to 60 T with a pulse duration in the one second range [35], sometimes described as quasi-static.…”
Section: Review Of the Existing High Magnetic Field Systemsmentioning
confidence: 99%
“…Pulsed magnetic fields up to 32 T were generated by the discharge (up to 1.25 MJ) of a capacitor bank (25,000 mF) into a resistive copper coil immersed in liquid nitrogen. The wave form of the increasing field is a quarter of a sine wave and the maximum is reached in 75 ms, the magnetic field then decreases to 0 in 1.3 s following an exponential law due to crowbar diodes [35] inserted in the circuit, see Fig. 1.…”
Section: Review Of the Existing High Magnetic Field Systemsmentioning
confidence: 99%
“…The pulse shape is a damped sine wave distorted by the heating of the coil. It is common practice to connect a 'crowbar' circuit, consisting of a resistor and a diode, in parallel to the capacitor bank [3]. The 1 Present address: Forschungszentrum Rossendorf e.V., Postfach 510119, D-01314, Dresden, Germany.…”
Section: Introductionmentioning
confidence: 99%