共查询到20条相似文献,搜索用时 20 毫秒
1.
M. Tarafder I. Chattoraj A. Mitra 《Journal of magnetism and magnetic materials》2009,321(8):1034-1038
The general trend of magnetic behaviour of materials is that the mechanically hard materials are also magnetically hard. However for the high strength low alloy (HSLA) steel tempered at various aging temperatures, the correlation was reported as negative. The anomaly could not be explained by the magnetic parameters like RMS voltage calculated from the Barkhausen emission signal and the coercivity from the magnetic hysteresis loop. This paper reports another magnetic parameter known as power-law decay exponent which shows excellent correlation with the mechanical properties and thus explains the progressive evolution of the microstructural constituents in HSLA steel. 相似文献
2.
We have studied similarity rules of quasistatic minor hysteresis loops for Fe and Ni single crystals in the wide temperature range from 10 to 600 K. Two similarity rules of MR*/Ma*∼3/4 and WR*/WF*∼1/6, were found in a medium field range where irreversible movement of Bloch walls plays a crucial role for magnetization; Ma*, MR*, WF*, and WR* are magnetization, remanence, hysteresis loss, and remanence work of a minor hysteresis loop. The similarity rules hold true, being almost independent of kinds of ferromagnets, applied stress, and temperature. The origin was discussed from the viewpoint of pinning effects due to dislocations as well as eddy current effects which become predominant at low temperatures for samples with low dislocation density. 相似文献
3.
Recoil hysteresis and temperature dependence of coercivity have been measured for the sample of composition Nd4Fe73.5Co3Hf0.5Ga0.5B18.5 prepared by rapid quenching method with a wheel speed of 25 m/s and after subsequent annealing in an evacuated quartz tube under a pressure of 10–5 mbar at different temperatures and times. In the optimum and over‐annealed condition, recoil hysteresis loops have been measured by the application of progressively increasing negative field and successive withdrawal to the remanence and found to have steep recoil loop and small recoil area, which is characteristic to exchange‐biased system. Temperature dependence of coercivity in the range of 5 K to 380 K has been measured for the sample of composition Nd4Fe73.5Co3Hf0.5Ga0.5B18.5. Variation in the shape of the hysteresis loop has been observed in this temperature range. In the low temperature region i.e. below 150 K hysteresis loops are constricted due to spin reorientation of Nd2Fe14B at 135 K while above this temperature the hysteresis loops are characterized by convex M (H) curve similar to single‐phase permanent magnet. (© 2008 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
4.
An amorphous alloy of composition (NdPr)4Fe71Co5Cu0.5Nb1B18.5 prepared by a melt spinning technique in an argon atmosphere has been studied to observe exchange‐spring behavior in the nanocrystalline state. Hysteresis loop measurements at room temperature revealed that the highest value of the coercivity, Hc, of 4.08 kOe has been obtained for the sample annealed at 913 K for 10 min. At this annealing temperature (BH)max and Mr/Ms have been found to be 11.06 MGOe and 0.716, respectively. Steep recoil curves of the samples annealed at 873 and 973 K show typical characteristics of the exchange‐spring mechanism having smaller loop area. The temperature dependences of Hc, Mr/Ms and (BH)max in the range of 5 to 380 K generally decrease with the increase of temperature. From the temperature dependence of the hysteresis loop parameters, it has been found that at 5 K the values of Hc and (BH)max are 6.89 kOe and 13.72 MGOe respectively for the sample annealed at 873 K for 10 min and 6.69 kOe and 13.74 MGOe respectively for the sample annealed at 923 K for 10 min. A change in the shape of the hysteresis loops was observed at temperatures below 100 K, related to the spin reorientation in the hard magnetic phase. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
5.
Seok-Soo Yoon N.A. Buznikov Lan Jin Chong-Oh Kim CheolGi Kim 《Journal of magnetism and magnetic materials》2006
The off-diagonal magnetoimpedance in field-annealed CoFeSiB amorphous ribbons was measured using a pick-up coil wound around the sample. One side of a ribbon was etched in hydrofluoric acid solution during various times in order to change the thickness of the surface crystalline layer appearing after annealing. The asymmetric two-peak field dependence of the off-diagonal impedance was observed for all samples. The evolution of the off-diagonal magnetoimpedance with the change in the ribbon thickness is analyzed. 相似文献
6.
Sergey E. Zirka Yury I. Moroz Philip Marketos Anthony J. Moses 《Journal of magnetism and magnetic materials》2008
The loss predictive methods based on the static and dynamic components of power loss are compared with the methods where the total loss is subdivided into hysteresis, classical and excess components. It is explained why the simplest two-component methods can be preferable. An approach to the characterization of a given steel is outlined. 相似文献
7.
K. S. Ryu Youn‐Ju Park C. G. Kim Je Cheon Ryu D. Son 《physica status solidi (a)》2004,201(8):1815-1818
To reduce the core loss of grain oriented silicon steel, various metallurgical attempts have been made. The laser scribing reduces the core loss of 3% Si–Fe, because sub‐domains induced by scribing produce many active domain walls which reduce the eddy current loss. The profiles of ac hysteresis loop and core loss have been measured for samples oriented parallel and perpendicular to the [001] axis in (110)[001] grains of 3% Si–Fe before and after laser scribing. The observed ac hysteresis loop profiles have been analyzed in terms of domain reorientation under field. For the parallel and perpendicular samples, the reductions of core loss are 5.7% and 30.3% by laser scribing at the magnetic induction 1.3 T and magnetizing frequency 60 Hz. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
8.
NdFeNbB with the additions of Dy2O3 and Sn permanent magnets have been attained by means of powder-blending technique, and their magnetic properties, temperature performance and microstructure were studied in this paper. The addition of just 2.0 wt% Dy2O3 or 0.3 wt% Sn proved to be very effective in improving the permanent magnetic properties of NdFeNbB magnets. Dy2O3 additions result in the increase in the Hci and temperature dependence due to the increase of Tc, formation of (NdDy)-rich phase and grain refinement of Φ phase. This improvement of the coercivity stability of the magnets from the addition of Sn is attributed to the smoothing effect of the Sn addition at the grain boundaries. The magnetic properties, the temperature dependence and Curie temperature of NdFeNbB with Dy2O3 and Sn combined addition were found to be considerably improved. From the X-ray diffraction, SEM-EDAX studies and the thermo-magnetic study, the improved properties due to the solution of Dy and Sn to the Φ phase, the reduced Neff and the smaller Φ phase. 相似文献
9.
K. S. Ryu Youn‐Ju Park Y. B. Kim Je Cheon Ryu D. Son 《physica status solidi (a)》2004,201(8):1819-1822
The profiles of ac hysteresis loops have been measured as function of the angle ϕ between H‐field and [001] axis in (110)[001] grain oriented 3% silicon‐iron. As ϕ increases, for ϕ ≥ 30° the loop changes into a wasp‐waisted shape with inflection points. The observed ac hysteresis loop profiles have been analyzed in terms of domain reorientation under field. The core losses in silicon‐iron are measured for various magnetizing angles with respect to the easy axis at magnetizing frequency 50 Hz and 60 Hz and at magnetic induction 1.3 T and 1.0 T. At magnetic induction 1.3 T, the core loss increased to near 70° and decreased at magnetizing frequency 60 Hz, but at 50 Hz this trend was different from 60 Hz and the core loss was monotonously increased. (© 2004 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
10.
The main subject of this work was to analyze magnetic losses of non-oriented soft magnetic materials, which are used in rotating machines like motors or generators, under the conditions of alternating and rotating magnetic flux. For this purpose a hexagonal rotational single sheet tester (HRSST) and a standardized 25 cm Epstein frame tester (EFT) were used, respectively. Since each HRSST sample represents only one random sample, whereas a stack of EFT samples represents a basic population of a production lot, a simple procedure is introduced to derive characteristic rotational loss data from EFT measurements and previously acquired loss factors. 相似文献
11.
Magnetization curves of untreated and laser scribed GO FeSi steels were measured for 19 different frequencies from 0.05 to 500 Hz and for four polarizations from 1.4 to 1.7 T. From hysteresis loops, hysteresis losses were separated and frequency-dependent anomaly factors were calculated. Frequency-dependent anomaly factors for all measured polarizations can be very well described by an empirical equation. This behavior can be explained by the fact that an increase in polarization at a fixed magnetizing frequency corresponds to an increase of magnetizing frequency at a fixed polarization. Both an increase in frequency and an increase in polarization activate a higher number of domain walls in the magnetization process. The power losses can be described only by the frequency dependence of the anomaly factor and by the additional knowledge of hysteresis loss. 相似文献
12.
A “Lean Grade Policy” has been adopted involving reduced losses of a given steel composition and supplied grades with typical losses closer to the guarantees. Increased final annealing temperatures and modified hot rolling have resulted in reduced losses and improved permeability. A “lean grade” will have higher heat conductivity and permeability compared to a “standard grade”. The policy could result in less variability and better quality control. 相似文献
13.
The power losses of a non-oriented 3% Si-steel rolled to gauges between 0.05 and 2 mm and heat-treated thereafter have been measured under sinusoidal polarizations at frequencies between 15 Hz and 10 kHz. The losses were analysed using a loss separation model based on statistical theory. For the thick samples the skin effect caused the model to fail above a certain frequency, while for the very thin samples the model seems to describe the losses well at all frequencies studied. 相似文献
14.
G.A. Badini-Confalonieri G. InfanteJ. Torrejón M. Vázquez 《Journal of magnetism and magnetic materials》2008
We report on the magnetic behaviour of a novel family of two-magnetic-phase multilayer microwires consisting of: (i) a bistable FeSiB glass-coated amorphous microwire as soft nucleus, and (ii) a polycrystalline CoNi outer microtube as harder layer. Such bi-phase microwires are prepared by combined quenching and drawing plus sputtering and electroplating techniques. The stray field produced by the harder outer layer after premagnetizing it to saturation is used to bias the magnetization reversal process of the soft nucleus via dipolar magnetostatic coupling. A detailed analysis of the asymmetric low-field magnetization reversal process of the soft nucleus is presented together with the study of the fluctuating switching field and its asymmetric behaviour. The study of the domain wall characteristics under the presence of a nucleation coil at one end of the microwire allows us to draw conclusions on the role of the bias field generated by the premagnetized hard outer layer. 相似文献
15.
Jesús Daniel Santos lvaro Ruiz Raúl F. Cobos Ivn Ribot Víctor Vega Pablo lvarez María Luisa Snchez Jos Luis Snchez Ll. Víctor M. de la Prida Blanca Hernando 《physica status solidi (a)》2009,206(4):618-621
The influence of glass covering on domain wall propagation in Fe65B15Si15C5 amorphous microwires is studied, before and after glass removal. High values of domain wall velocity and mobility have been obtained. The domain wall velocity depends linearly on the driving magnetic field. However, the mobility of the domain wall is very different in both situations studied. The results are explained due to the modification of internal stress distribution after glass removing, that change the domain structure of the sample. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
16.
M. Kisielewski Z. Kurant M. Tekielak W. Dobrogowski A. Maziewski A. Wawro L. T. Baczewski 《physica status solidi (a)》2003,196(1):129-132
Ultrathin cobalt wedges Au/Co(0 < d < 2 nm)/Au(111)/Mo/Al2O3, grown by molecular beam epitaxy, were investigated by means of the polar Kerr effect. Coercivity field HC as a function of Co film thickness d was determined from the hysteresis loops. Domain structure in the remnant states, affected by a magnetic history of the sample, were investigated by optical polarizing microscope equipped with a computer controlled CCD camera. Both domain nucleation center maximum density, nmax(d), registered during magnetization reversal process and wall fractal dimension, fd(d), were determined by digital images processing. Increasing d, a rapid increase of both nmax and fd was observed approaching the magnetization reorientation phase transition from easy axis into easy plane. Similar strong changes were observed while decreasing d for the lowest thickness available for observation. 相似文献
17.
Modern passenger cars are increasingly equipped with electromechanical steering assist rather than hydraulic systems known for many decades. Major benefits are reduced fuel consumption (up to 0.2l/100 km) and increased functionality. As such a system reacts to the drivers input in terms of steering torque or steering effort, a sensor is required that accurately measures the steering torque. Valeo has adopted a magnetic technology and has improved the performance by adding specially designed flux concentration devices. The magnetic circuit consists of a multi-pole ring magnet and a pair of ring-shaped soft magnetic parts rotating together with the steering shaft and an additional pair of soft magnetic flux concentration devices which are fixed stationary inside the housing. The steering torque causes a relative twist between magnet and the soft magnetic rings, therefore implementing a proportional magnetisation of the latter. A U-shape was chosen for the flux concentration devices in order to compensate mechanical tolerances of the system. The main focus of this paper will be on the tolerance behaviour of the sensor system and the impact of the flux concentration devices. Because of the nonlinear nature of the magnetisation curve of the NiFe alloy used extensive 3D FEM simulation was necessary. Simulation enables us to have a look inside the soft magnetic material and predict the spatial magnetisation distribution with the benefit of avoiding saturation. The result is an optimised sensor, which meets both the harsh environmental conditions inside the motor compartment as well as the cost pressure in the automotive business. 相似文献
18.
Germn Infante Jacob Torrejn Karla J. Merazzo G. A. Badini‐Confalonieri Manuel Vzquez 《physica status solidi (a)》2009,206(4):622-624
The dynamic (AC) switching field in the soft FeSiB bistable nucleus of the Fe77.5Si7.5B15–Co90Ni10 bi‐phase microwires family has been measured over the frequency range 20 Hz to 2 kHz. Microwires with a CoNi thickness ranging between 0.5 μm and 8 μm were studied. Results are well fitted by a power law dependence of the switching field H * on magnetic field frequency f. As the thickness of the harder CoNi outer shell is increased, the parameters which characterise the best fit experience noticeable changes. The origin of such behaviour is interpreted in terms of modifications in the soft FeSiB nucleus domain structure, accordingly to previous established models. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
19.
The exchange field is found to change as an exponential function of 1/|t1 — t2| in two wedged synthetic antiferromagnets FeMn/Co(t1 = 12.0 nm)/Ru(0.7 nm)/Co(t2) and FeMn/Co(t1)/Ru(0.7 nm)/Co(t2 = 12.0 nm). It has opposite signs and different magnitudes in the two above series. Based on a simple model of magnetization, coherent rotation and magnetically non‐rigid coupling, numerical calculations showed that this asymmetrical and exponential dependence is attributed to a non‐collinear alignment of the magnetizations in the low field range. It is interesting to find that the minor loop has a pronounced asymmetrical shape when the two ferromagnetic layers are close in thickness, hinting the formation of a planar domain wall in the FeMn layer during the magnetization reversal of the ferromagnetic layers. 相似文献
20.
Thomas Jourdan Frédéric Lançon Laurent Vila 《Journal of magnetism and magnetic materials》2009,321(14):2187-2191
FePt thin layers have been epitaxied either on Pt(0 0 1) or on MgO(0 0 1) substrates, and magnetically characterized using extraordinary Hall effect magnetometry and magnetic force microscopy. The coercivity originates in both cases from the pinning of domain walls on structural defects. Whereas the coercivity increases with the FePt layer thickness in FePt/Pt samples, it decreases in FePt/MgO samples. This discrepancy is explained on the basis of structural observations, and of atomistic simulations of magnetic domain wall pinning. 相似文献