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The Effect of Structural Changes on Magnetic Permeability of Amorphous Powder Ni_(80)Co_(20)

机译:结构变化对非晶态粉末Ni_(80)Co_(20)磁导率的影响

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The structural changes of Ni_(80)Co_(20) amorphous powder were tested during heating. The alloy was obtained by electrolysis from ammonia solution sulfate of cobalt and nickel on the titanium cathode. The differential scanning calorimetry (DSC) method was used to detect that the crystallization process of powder occured in two stages with crystallization peaks temperatures of the first stage at 690 K and of the second stage at 790 K. The effect of structural relaxation and crystallization of powder on magnetic properties was predicted by measurement of the relative magnetic permeability change in isothermal and nonisothermal conditions. On the basis of the time change of relative magnetic permeability at a defined temperature in the temperature range of the first and second crystallization peak pn the thennogram, the kinetics of crystallization was defined. It was predicted, that in the initial time interval, in the range of the first crystallization peak, the rate of crystallization is determined by the rate of nucleation of the amorphous part of the powder. However, in the second time interval, the crystallization rate is determined by the rate of diffusion. In the range of the second peak, in the beginning the rate of crystal growth is determined by activation energy of the atom pass from smaller to bigger crystal grain. In second time interval, the rate of crystal grain growth is determined by the diffusion rate of atoms to the location of integration into bigger crystal grains. For all processes which determine the rate of crystallization in temperature ranges of both crystallization peaks, the Arrhenius temperature dependence of rate for those processes is obtained. The relative magnetic permeability of crystallized powder at 873 K, is smaller for about 30 percent than the relative magnetic permeability of fresh powder at room temperature. However, structurally relaxed powder at 573 K has an about 22 percent larger magnetic permeability than the same fresh powder at room temperature.
机译:在加热过程中测试了Ni_(80)Co_(20)非晶态粉末的结构变化。该合金是通过在钛阴极上从钴和镍的氨硫酸盐溶液中电解得到的。用差示扫描量热法(DSC)检测粉末的结晶过程分两个阶段发生,第一阶段的结晶峰温度为690 K,第二阶段的结晶峰温度为790K。通过测量等温和非等温条件下的相对磁导率变化来预测粉末的磁性能。基于第一结晶峰和第二结晶峰的温度范围内的限定温度下的相对磁导率随时间的变化,定义了结晶动力学。据预测,在初始时间间隔内,在第一结晶峰的范围内,结晶速率由粉末的非晶态部分的成核速率决定。然而,在第二时间间隔中,结晶速率由扩散速率确定。在第二个峰的范围内,开始时晶体生长的速度取决于原子从较小晶粒到较大晶粒的活化能。在第二时间间隔中,晶粒的生长速率由原子向集成到较大晶粒中的位置的扩散速率确定。对于在两个结晶峰的温度范围内确定结晶速率的所有过程,都获得了这些过程的速率的阿伦尼乌斯温度依赖性。结晶粉末在873 K时的相对磁导率比新鲜粉末在室温下的相对磁导率小约30%。但是,在573 K下结构松弛的粉末在室温下的磁导率比相同的新鲜粉末大22%。

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