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Fe16N2: from a 40-year mystery of magnetic materials to one of promises for rare-earth-free magnets.

机译:Fe 16 N 2 :从40年的磁性材料之谜到无稀土磁体的应许之一。

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摘要

Fe16N2 is one of the most promising rare-earth-free magnet candidates with high magnetic energy product. Iron nitride magnet is of great interest as a magnetic material for applications at relatively low temperature (<;150 <;°C) ranging from magnets in hard disk drives for data storage and in all kinds of electrical motors, wind turbines, and other power generation machines. A perspective review on our research work on bulk Fe16N2 compound permanent magnet in past years is presented on the aspects of material processing and magnetic characterizations. Specifically, we will introduce and discuss our effort to prepare bulk Fe16N2 compound permanent magnet by using three different approaches, including an ion implantation method, a ball milling method and a strained-wire method. A feasibility of free-standing iron nitride foils with magnetic energy product up to 20 MGOe was successfully demonstrated based on an ion implantation method. Based on our theoretical and experimental progress, we believe that Fe16N2 compound permanent magnet is currently in an accelerating step to be an alternative magnet candidate. TECHNICAL RESULTS AND DISCUSSION: During past decades, several permanent magnet materials were discovered, especially those based on rare-earth intermetallic compounds [1,2,3]. The key fi gure of merit of permanent magnets is the energy product (BH) . Figure 1 lists the development in the maximum magnetic energy product (BH) at room temperature of market -available hard magnetic materials so far [4] and our predicted value for iron nitride magnet. It is interesting to note that this value, starting from 1MGOe for steels discovered during the early part of last century, increasing to 3MGOe for ferrites, and finally that peaks at 56MGOe for ueodymium-iron-boron magnets during the past twenty years. However, new magnets with more abundant and less economically-limited and environmentally -restricted elements is highly demanded to supplement rare earth magnets [3]. At the same time, the saturation magnetization of rare earth magnets may not be high enough to satisfy the requirements for the applications of electric machines. One of basic function of permanent magnets used in electric vehicles and wind turbines is to provide magnetic flux. This function requires a higher saturation magnetization as well as an appropriate coercivity to against self -demagnetization. The most ideal permanent magnet should have the following features: (1) be composed by abundant and environment friendly elements; (2) large saturation magnetization; (3) large energy product; (4) reasonable high coercivity; (BH)max has doubled every 12 years during the 20th century mainly with the progress due to improvements in coercivity [4]. Next generation permanent magnet would be expected with a higher remanent magnetization while with a reasonable coercivity. Fe 16N2 has been viewed as a controversial material or mystery before 2000. We have started to work on this material since 2003. Besides reporting a systematic experimental study on Fe16N2 thin films and confirmed its giant saturation magnetization and large anisotropy constant [5], we proposed a "cluster + atom" model based on the fi rst -principles calculation to explain the giant saturation magnetization of Fe16N2 [6]. This model is supported by the discovery of partially localized 3d electrons in Fe16N2 [5]. After those validations, Fe16N2, with a magnetic flux density as high as 2.9T and an anisotropy constant up to 1.0-1.8 MJ/m 3 [7] has been expected to be one of possible ram -earth -free magnet candidates. Moreover, Fe16N2 has combined features of low cost with most redundant elements on earth, environment -friendly and theoretically two times higher energy product than the current market available rare earth magnets, as shown in Fig. 1. In this paper, we introduce three approaches, including an ion implantation approach, a strained -wire method and a ball milling method, which we developed in past six years, for the synthesis of bulk Fe16N2 magnets. By using a nitrogen ion implantation approach [8], we successfully synthesized free-standing Fe16N2 foils with a coercivity of up to 1910 Oe and a magnetic energy product of up to 20 MGOe at room temperature. An integrated synthesis technique was developed, including a direct foil-substrate bonding step, an ion implantation step and a two-step post-annealing process. With the tunable capability of the ion implantation fluence and energy, a microstructure with grain size 25-30 nm is constructed on the FeN foil sample with the implantation fluence of 5×1012/cm2. To the best of our knowledge, this could be the first experimental evidence of the existence of a giant saturation magnetization, an obviously large coercivity with a magnetic energy product of up to 20 MGOe in a bulk -type FeN magnet sample. Ball milling is one of the other approaches to prepare the Fe16N2 Powder [9]. Shock compaction using a gas gun was used to compact the powder into a dense disk shape. We experimentally demonstrated that the volume ratio of the Fe16N2 phase is 70% and that it is stable under shock compaction, without obvious phase decomposition. This approach presents the possibility of mass producing bulk permanent magnets using Fe16N2 with enhanced magnetic properties. Furthermore, we proposed and demonstrated a novel synthesis method for bulk anisotropic Fe16N2 magnet, named as the "strained wire method" [10]. Based on this method, an anisotropic bulk iron nitride magnet with 9 MGOe was achieved for the first time.
机译: 16 ñ 2 是具有高磁能积的最有前途的稀土候选磁体之一。氮化铁磁铁作为一种磁性材料,在相对低温(<; 150 <;°C)的应用中引起了极大的兴趣,其范围从硬盘驱动器中的磁铁用于数据存储,以及在各种电动机,风力涡轮机和其他电源中一代机器。关于我们对散装铁的研究工作的观点回顾 16 ñ 2 在材料加工和磁特性方面介绍了近年来的复合永磁体。具体来说,我们将介绍和讨论我们准备大块铁的工作 16 ñ 2 通过使用三种不同的方法合成复合永磁体,包括离子注入法,球磨法和拉丝法。基于离子注入方法,成功证明了磁能积高达20 MGOe的自支撑氮化铁箔的可行性。根据我们的理论和实验进展,我们认为铁 16 ñ 2 复合永磁体目前正处于加速发展阶段,成为替代磁体的候选者。技术结果与讨论:在过去的几十年中,发现了几种永磁材料,尤其是那些基于稀土金属间化合物的永磁材料[1,2,3]。永磁体的主要性能指标是能量积(BH)。图1列出了迄今为止市场上可用的硬磁材料在室温下最大磁能积(BH)的发展情况[4],以及我们对氮化铁磁体的预测值。有趣的是,这个值从上世纪初发现的钢材的1MGOe开始,到铁氧体的这个值增加到3MGOe,最后在过去的20年中,铁-铁-硼磁铁的峰值达到56MGOe。然而,人们强烈要求新型磁铁具有更多,经济上的限制和对环境的限制,以补充稀土磁铁[3]。同时,稀土磁体的饱和磁化强度可能不足以满足电机应用的要求。电动汽车和风力涡轮机中使用的永磁体的基本功能之一是提供磁通量。此功能需要较高的饱和磁化强度和适当的矫顽力,以防止自磁化。最理想的永磁体应具有以下特征:(1)由丰富且环保的元素组成; (2)饱和磁化强度大; (3)大型能源产品; (4)合理的高矫顽力; (BH) max 在20世纪每12年翻一番,这主要是由于矫顽力的提高所致[4]。下一代永磁体将具有更高的剩余磁化强度和合理的矫顽力。铁 16 ñ 2 在2000年之前一直被视为有争议的材料或谜团。我们从2003年开始研究这种材料。除了报道对铁的系统性实验研究之外, 16 ñ 2 薄膜,并确认其巨大的饱和磁化强度和大的各向异性常数[5],我们提出了一种基于第一个预期计算的“集群+原子”模型,以解释Fe的巨大饱和磁化 16 N 2 [6]。该模型得到FE中的部分局部3D电子的发现支持 16 N 2 [5]。在这些验证之后,FE 16 N 2 ,预计磁通密度高达2.9T的磁通密度高达1.0-1.8MJ / m 3 [7]的各向异性恒定是可能的RAM -Free磁铁候选者之一。而且,Fe. 16 N 2 在地球上的大多数冗余元素具有低成本的综合特征,环境友好和理论上的能量产品高于当前市场可获得的稀土磁铁,如图1所示。在本文中,我们介绍了三种方法,包括一个离子植入方法,一种紧张的丝网法和六年级开发的球磨方法,用于批量FE的合成 16 N 2 磁铁。通过使用氮离子植入方法[8],我们成功地合成了独立式Fe 16 N 2 箔,矫顽力高达1910°OE和室温下可达20mgee的磁能产物。开发了一种综合的合成技术,包括直接箔基板键合步骤,离子注入步骤和两步后退火过程。通过离子注入能量和能量的可调谐能力,在芬箔样品上构建具有晶粒尺寸25-30nm的微观结构,其中植入量为5×10 12 /厘米 2 。据我们所知,这可能是巨型饱和磁化强度存在的第一个实验证据,这是一个明显大的矫顽力,其磁性能量在散装磁铁样品中最多20 MGOE。球磨是准备FE的其他方法之一 16 N 2 粉末[9]。使用燃气枪的冲击压实将粉末压缩成致密的盘形。我们通过实验证明了FE的体积比 16 N 2 阶段是70%,并且在休克压实下它是稳定的,没有明显的相位分解。这种方法呈现了使用Fe生产块状永磁体的可能性 16 N 2 具有增强的磁性。此外,我们提出并展示了散装各向异性Fe的新型合成方法 16 N 2 磁铁,被命名为“紧张导线法”[10]。基于该方法,首次实现了具有9mgOe的各向异性散装铁氮化物磁铁。

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