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首页> 外文期刊>Journal of Applied Physics >Study of Magnetic Losses at Low Flux Densities in 35 Permalloy Sheet
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Study of Magnetic Losses at Low Flux Densities in 35 Permalloy Sheet

机译:35坡莫合金薄板低通量密度下的磁损耗研究

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Energy losses in ferromagnetic materials subject to alternating fields have long been considered as due solely to hysteresis and eddy currents. However, at the low flux densities encountered in certain communication apparatus, a further loss is observed which has been variously termed ``residual,'' ``magnetic viscosity,'' or ``square law hysteresis.'' The search for an explanation of this loss has led to precise measurements of hysteresis loops with a vacuum ballistic galvanometer, and of a.c. losses with inductance bridges. From these results, it appears that that part of the a.c. effective resistance of a coil on a ferromagnetic core which is proportional to the coil current is strictly identified with the hysteresis loop area as measured by a ballistic galvanometer, or as indicated by harmonic generation in the coil. The hysteresis loop can now be constructed in detail as to size and skewness on the basis of a.c. bridge measurements. This conclusion was reached previously on a compressed iron powder core, and is now confirmed on an annealed laminated 35 permalloy core. Observed eddy current losses for this core exceed those calculated from classical theory by 20 percent. This excess is ascribed to the presence of low permeability surface layers on the sheet magnetic material. The a.c. residual loss per cycle (nominally independent of frequency, like hysteresis) is not observed by ballistic galvanometer measurements, although it indicates an energy loss some eight times the hysteresis loss for the smallest loop measured (Bm = 1.3 gauss). Analysis of the residual loss shows that it increases with frequency up to about 500 cycles, and remains constant at higher frequencies (to 10,000 cycles per second). Concurrently with the increase of residual loss, the permeability of the alloy is observed to decline with increasing frequency about 1 percent below the value predicted from eddy current shielding. This effect is most noticeable at frequencies below-n 1000 cycles.
机译:长期以来,人们一直认为铁磁材料中的能量损耗是由于磁滞和涡流引起的。但是,在某些通信设备中遇到的低通量密度时,会观察到进一步的损耗,这些损耗已被不同地称为``残余'',``磁粘性''或``平方律磁滞''。的损耗导致了用真空弹道振镜精确测量磁滞回线和交流电感桥的损耗。从这些结果看来,交流的那一部分铁磁芯上的线圈的有效电阻与线圈电流成正比,严格地由磁滞振镜测量的磁滞回线面积确定,或者由线圈中的谐波产生指示。现在可以根据交流电来详细构造磁滞回线的大小和偏度。桥梁测量。先前在压缩铁粉磁芯上得出了这一结论,现在在退火的层压35坡莫合金磁芯上得到了证实。观察到的该铁心的涡流损耗比经典理论计算的涡流损耗高20%。该过量归因于薄磁性材料上存在低磁导率表面层。交流弹道电流计测量未观察到每个周期的残余损耗(名义上与频率无关,如磁滞),尽管它表示的能量损耗约为最小环路(Bm = 1.3高斯)的八倍。对残余损耗的分析表明,它随频率增加而增加,直至大约500个周期,并且在较高频率下保持恒定(每秒10,000个周期)。同时,随着残余损耗的增加,合金的磁导率随频率的增加而下降,该频率比涡流屏蔽预测的值低约1%。在低于-n 1000个周期的频率上,这种影响最为明显。

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  • 来源
    《Journal of Applied Physics 》 |1937年第5期| 共8页
  • 作者

    Ellwood W. B.; Legg V. E.;

  • 作者单位

    Bell Telephone Laboratories, New York, N. Y.;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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