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Jahn, L.; Schumann, R., E-mail: schumann@theory.phy.tu-dresden.de2002
AbstractAbstract
[en] The dependence of the thermal remagnetization (TR) in sintered hard magnets on external magnetic fields has been investigated in order to determine more precisely the grain-interaction fields in the DC-demagnetized state. That negative external field at which the TR or its initial slope vanishes or changes its sign, corresponds well to the theoretical parameter σf, i.e. the distribution width of internal field fluctuations. For the 'normal' TR of the metallic magnets SmCo5, Sm2Co17 and NdFeB these fields are of the order of -0.5, 0.25 and -0.04 T, respectively. For the 'inverse' TR at the hard ferrites this external field is about -0.02 T. The systematic variation of the TR-curves with a small external field is well explained by our theoretical model and leads to a refinement of the parameters for SmCo5 and barium ferrite. Susceptibility measurements with small alternating fields, carried out at different points of the TR curve, as well as repeating TR-experiments at SmCo5 demonstrate clearly that the TR is mainly due to the contribution of the 'weak' grains, remagnetizing in the interaction fields of the 'hard' grains
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Source
S0304885302004833; Copyright (c) 2002 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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Schumann, R.; Jahn, L., E-mail: schumann@theory.phy.tu-dresden.de2001
AbstractAbstract
[en] A self-consistent mean-field theory explaining the thermal remagnetization (TR) of polycrystalline permanent magnets is given. The influence of the environment of a grain is treated by an inclusion approximation, relating the field inside the grain to the local field outside by means of an internal demagnetization factor n. For the switching fields and the fluctuations of the local fields around the mean field, Gaussian distributions of widths σs, and σf, respectively, are assumed. The isothermal hysteresis curve, the recoil curves, and the TR dependent on the model parameters n, σs, and σf are calculated. Furthermore, the influence of the initial temperature and the strong dependence of the TR on the demagnetization factor of the sample are studied, and it is shown that for reasonable parameter sets TR effects up to 100% are possible. The theoretical results correspond well with the experimental situation
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Secondary Subject
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S0304885301001500; Copyright (c) 2001 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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AbstractAbstract
[en] Torque curves of SmCo5 sintered magnets with regularily lowered coercivity up to a maximum field H = 28 x 105 Am-1 have been registered automatically. From the observed rotational hysteresis the values of the rotational integral could be estimated in dependence on the degree of lowering of the coercivity. By comparison with theoretically calculated values for a simple nucleation model for a single crystal it follows that the mechanism of the magnetization reversal for SmCo5 magnets with lowered coercivity should be pinning of Bloch walls in the multidomain state. The absolute value of the maximum rotational hysteresis work is comparable with the maximum linear hysteresis work. (author)
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International symposium on magnetic properties of rare earth alloys; Varna (Bulgaria); 4-6 Oct 1982; Poster presentation.
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Journal Article
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Conference
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Wissenschaftliche Zeitschrift - Hochschule fuer Verkehrswesen Friedrich List, Dresden; ISSN 0043-6844; ; v. 30(4); p. 939-948
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AbstractAbstract
[en] The known process of the thermal remagnetization of SmCo5 is explained half quantitatively as a typical effect in a polycrystal by assuming a square spectrum of its coercivities and parallel orientation of its easy axes. Together with large (H/sub R/ - H/sub c/)-differences it is caused by a fluctuating interaction field H' combined with the irreversible reduction of the low coercivity side of the H/sub c/-spectrum. From the measured field dependence on SmCo5 as well as on BaFe12O19 magnets the field H' can be estimated experimentally and found to be H' = 0.3 and 0.5 x 105 Am-1 for a temperature T0 = 180 and 270 0C, respectively. (author)
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AbstractAbstract
[en] The torque T and the rotational hysteresis (rh) of permanent magnets with the composition Sm(Co/sub 0.65/Fe/sub 0.27/Cu/sub 0.06/Zr/sub 0.02/)/sub 7.44/ have been investigated at room temperature. T and rh depend sensitivity on the magnetization state of the magnet. A dependence of the rh work on the coercivity and the magnetic state of the material could be shown. Results give evidence that in the annealed samples the domain walls are easily movable where after the thermal treatment the hard magnetic characteristics of the sample are nearly recovered
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Short note.
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Journal Article
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Physica Status Solidi. A, Applied Research; ISSN 0031-8965; ; v. 83(2); p. K141-K144
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Jahn, L.; Ivanov, V.; Schumann, R.; Loewenhaupt, M., E-mail: schumann@theory.phy.tu-dresden.de2003
AbstractAbstract
[en] Modern permanent magnets show an irreversible increase of the remanent magnetization for increasing temperature. This thermal remagnetization (TR) occurs after DC-demagnetization at the initial temperature T0 followed by heating. The TR is especially large for well-aligned sintered SmCo5 permanent magnets and is strongly correlated with the grain-interaction and the temperature coefficient of the coercivity. We present a systematical study on the influence of the initial temperature T0 on the TR of SmCo5 sintered magnets experimentally and theoretically. We find that the TR-maximum increases with decreasing T0, whereas its position Tmax shifts slightly to lower temperatures with decreasing T0. This together with the dependence on the sample demagnetization factor N, is in agreement with the results of our model calculation
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S0304885302000197; Copyright (c) 2002 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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AbstractAbstract
[en] A simplified method for preparing sintered samarium-cobalt magnets without applying high pressures is presented. Depending on the samarium content and the course of sintering, relative densities up to 99 per cent could be reached. The limits of the method are given and possibilities for improvements are shown. (author)
Original Title
Schwachgepresste SmCo5-Sintermagnete
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Journal Article
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Neue Huette; ISSN 0028-3207; ; v. 24(5); p. 188-191
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AbstractAbstract
[en] The effect of 'thermal remagnetization' as a function of the positive applied field has been studied in two different technical 2:17 magnets: Sm2(Co0.65Fe0.27Cu0.06Zr0.02)14.9 and Sm2(Co0.709Fe0.205Cu0.06Zr0.02)15.5. After a thermal demagnetization of the samples the field has been increased to H and the magnetization M1 has been measured. Then the field has been decreased to -Hc and -HR and the coercivities Hc and HR have been measured. In a zero field the temperature was then increased to T1 and decreased to T0 and the magnetization increase ΔM has been registered. Two different types of virgin and remanence curves have been found. The values of Hc, HR, (HR - Hc), and normalized ΔM as functions of external saturation field are plotted and discussed
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Short note.
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AbstractAbstract
[en] The optical generation of coherent surface acoustic waves (SAW) is shown up to frequencies as high as 2 GHz on semiconductor surfaces. The frequency response of the acoustic coherence is directly related to thermal relaxation processes within the surface layer. Propagation of the optically generated SAW is shown to be sensitive to phase restructuring that occurs at solid-liquid interfaces
Source
3. international laser science conference: advances in laser science; Atlantic City, NJ (USA); 1-5 Nov 1987; CONF-871147--
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AbstractAbstract
[en] In order to test the model assumptions on hard magnetic properties of sintered NdFeB magnets, a comparison of the measured and calculated values of the magnetization and remanence coercivities HC and HR, respectively, as a function of the angle between texture axis and external field θ in Nd16Fe76B8 and (Nd0.9Tb0.1)16Fe76B8 is given and explained qualitatively
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Short note.
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