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Influence of heat treatment on the magnetic and piezomagnetic properties of amorphous and nanocrystalline Fe64Ni10Nb3Cu1Si13B9 alloy strips

机译:热处理对非晶态和纳米晶态的Fe64Ni10Nb3Cu1Si13B9合金带材的磁和压磁性能的影响

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FINEMET type alloy with substitution of 10 at.% of iron by nickel is studied from the point of view of the influence of the nanocrystallization process on the magnetic and magnetoelastic properties. Strip-shape samples of Fe64Ni10Nb3Cu1Si13B9 amorphous alloy were annealed in vacuum for I h in the temperature range of 350-550degreesC. Hysteresis loops were measured in order to determine the amount of anisotropy energy and corresponding anisotropy field, and coercive field of each annealed sample. This coercitivity reaches a minimum (about 5 A/m) after annealing at 460 degreesC. Magnetic field dependencies of magnetoelastic properties were also investigated. We have found a maximum value of the DeltaE effect and magnetomechanical coupling coefficient of 61% and 0.85, respectively, that are accompanied by a minimum value of the quality factor of about 2 for the sample annealed at 460 degreesC. Such good parameters are related with internal stress relief and structural relaxation of the samples. The subsequent drop of the magnetoelastic coupling coefficient for higher annealing temperatures is related directly with a drop on the magnetostriction value, from (22-26) x 10(-6) to 13 x 10(-6), due to the formation of a nanocrystalline structure in the samples. On the other hand, ultrasound velocities, measured at magnetic saturation of each sample, increase continuously between 4.9 and 5.6 km/s as the annealing temperature of the sample increases. (C) 2003 Elsevier B.V. All rights reserved. [References: 18]
机译:从纳米晶化过程对磁和磁弹性能的影响的角度出发,研究了用镍替代10%(原子)的铁的FINEMET型合金。 Fe64Ni10Nb3Cu1Si13B9非晶态合金的条状样品在350-550°C的温度范围内真空退火1小时。测量磁滞回线以确定每个退火样品的各向异性能的量以及相应的各向异性场和矫顽场。在460℃退火后,该矫顽力达到最小值(约5 A / m)。还研究了磁弹性特性的磁场依赖性。我们发现,在460℃退火的样品中,DeltaE效应的最大值和磁机械耦合系数分别为61%和0.85,同时伴随着品质因数的最小值约2。这样好的参数与内部应力释放和样品的结构松弛有关。较高退火温度下的磁弹性耦合系数的后续下降与磁致伸缩值的下降直接相关,从(22-26)x 10(-6)到13 x 10(-6),这是由于形成了样品中的纳米晶体结构。另一方面,随着样品退火温度的升高,在每个样品的磁饱和下测得的超声波速度在4.9 km / s和5.6 km / s之间连续增加。 (C)2003 Elsevier B.V.保留所有权利。 [参考:18]

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