...
首页> 外文期刊>Magnetics, IEEE Transactions on >Fe–Si–B–P–Cu Nanocrystalline Alloy Ribbons With High Saturation Magnetic Flux Density Prepared Using Industrial Materials
【24h】

Fe–Si–B–P–Cu Nanocrystalline Alloy Ribbons With High Saturation Magnetic Flux Density Prepared Using Industrial Materials

机译:使用工业材料制备的具有高饱和磁通密度的Fe–Si–B–P–Cu纳米晶合金带

获取原文
获取原文并翻译 | 示例
           

摘要

Magnetic properties and fine structure of Fe–Si–B–P–Cu nanocrystalline alloy ribbons have been investigated. The ${rm Fe}_{84.8}({rm Si},{rm B},{rm P})_{14}{rm Cu}_{1.2}$ alloy ribbons using industrial materials are produced by a single-roller melt-spinning method in air. The ${rm Fe}_{84.8}({rm Si},{rm B},{rm P})_{14}{rm Cu}_{1.2}$ nanocrystalline alloys exhibit low coercivity $H_{c}$ of 7–20 A/m in the compositional range of ${rm Si}=0hbox{--}2$ at% and ${rm P}=2hbox{--}8$ at% and high saturation magnetic flux density $B_{s}$ of 1.80 T or more in the compositional range of ${rm P}=0hbox{--}4$ at%. In particular, ${rm Fe}_{84.8}{rm Si}_{1}{rm B}_{10}{rm P}_{3}{rm Cu}_{1.2}$ nanocrystalline alloy annealed at 698 K exhibits both the high $B_{s}$ of 1.82 T and the low $H_{c}$ of 7.2 A/m. The iron loss $W$ at 50 Hz of the ${rm Fe}_{84.8}{rm Si}_{1}{rm B}_{10}{rm P}_{3}{rm Cu}_{1.2}$ nanocrystalline alloy is much smaller than oriented and nonoriented magnetic steel over the maximum induction $B_{m}$ range up to 1.7 T. In addition, nanocrystalline structure-n-n of the ${rm Fe}_{84.8}{rm Si}_{1}{rm B}_{10}{rm P}_{3}{rm Cu}_{1.2}$ alloy exhibits a homogeneous nanocrystalline structure composed of $alphahbox{--}{rm Fe}$ grains with 5–20 nm in diameter even using industrial materials. Therefore, the Fe–Si–B–P–Cu nanocrystalline alloy has good soft magnetic properties and a large economical advantage of low material cost by using industrial materials.
机译:研究了Fe–Si–B–P–Cu纳米晶合金薄带的磁性和精细结构。 $ {rm Fe} _ {84.8}({rm Si},{rm B},{rm P})_ {14} {rm Cu}使用工业材料的_ {1.2} $ 合金带材是通过单辊熔融纺丝法在空气中生产的。 <配方公式type =“ inline”> $ {rm Fe} _ {84.8}({rm Si},{rm B},{rm P})_ {14} {rm Cu} _ {1.2} $ 纳米晶合金的矫顽力低 $ H_ {c} $ 为7 –20 A / m,在 $ {rm Si} = 0hbox {-} 2 $ 的组成范围内 $ {rm P} = 2hbox {-} 8 $ at%和高饱和磁通密度 $ B_ {s} $ $ {rm P} = 0hbox {-} 4 $ at%。特别是 $ {rm Fe} _ {84.8} {rm Si} _ {1} {rm B} _ {10} {rm P} _ { 3} {rm Cu} _ {1.2} $ 纳米晶合金在698 K退火后表现出较高的 $ B_ {s} $ 为1.82 T,较低的 $ H_ {c} $ 为7.2 A / m 。 <公式公式类型=“ inline”> $ W $ > $ {rm Fe} _ {84.8} {rm Si} _ {1} {rm B} _ {10} {rm P} _ {3} {rm Cu} _ {1.2} $ >在最大感应范围内,纳米晶合金比取向和非取向电磁钢小得多,最大感应 $ B_ {m} $ 范围T.此外,<分子式> =“ inline”> $ {rm Fe} _ {84.8} {rm Si} _ {1} {rm B} _ { 10} {rm P} _ {3} {rm Cu} _ {1.2} $ 合金表现出由 $ alphahbox {-} {rm Fe} $ 晶粒,即使使用工业材料,其直径也为5–20 nm。因此,Fe–Si–B–P–Cu纳米晶合金具有良好的软磁性能,并且通过使用工业材料具有较低的材料成本,具有很大的经济优势。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号