摘要:
An R—Fe—B based thin film magnet including an R—Fe—B based alloy which contains 28 to 45 percent by mass of R element (where R represents at least one type of rare-earth lanthanide elements) and which is physically formed into a film, wherein the R—Fe—B based alloy has a composite texture composed of R2Fe14B crystals having a crystal grain diameter of 0.5 to 30 μm and R-element-rich grain boundary phases present at boundaries between the crystals. The magnetization characteristics of the thin film magnet are improved. The R—Fe—B based thin film magnet can be prepared by heating to 700° C. to 1,200° C. during physical film formation or/and the following heat treatment, so as to grow crystal grains and form R-element-rich grain boundary phases.
摘要翻译:包含R-Fe-B系合金的R-Fe-B类薄膜磁体,其含有28〜45质量%的R元素(其中R表示至少一种稀土镧系元素),并且其物理形成 其中R-Fe-B基合金具有由晶体直径为0.5至30μm的R 2 Fe 14 N 12 B晶体组成的复合纹理,以及 存在于晶体之间的边界处的富含R元素的晶界相。 提高了薄膜磁铁的磁化特性。 R-Fe-B类薄膜磁体可以在物理成膜或/和随后的热处理中加热至700℃至1200℃,从而生长晶粒并形成富含R元素的薄膜 晶界相。
摘要:
An R—Fe—B based thin film magnet including an R—Fe—B based alloy which contains 28 to 45 percent by mass of R element (where R represents at least one type of rare-earth lanthanide elements) and which is physically formed into a film, wherein the R—Fe—B based alloy has a composite texture composed of R2Fe14B crystals having a crystal grain diameter of 0.5 to 30 μm and R-element-rich grain boundary phases present at boundaries between the crystals. The magnetization characteristics of the thin film magnet are improved. The R—Fe—B based thin film magnet can be prepared by heating to 700° C. to 1,200° C. during physical film formation or/and the following heat treatment, so as to grow crystal grains and form R-element-rich grain boundary phases.
摘要翻译:包含R-Fe-B系合金的R-Fe-B类薄膜磁体,其含有28〜45质量%的R元素(其中R表示至少一种稀土镧系元素),并且其物理形成 其中R-Fe-B基合金具有由晶体直径为0.5至30μm的R 2 Fe 14 B晶体和存在于晶体之间的边界处的富R晶体相的复合结构。 提高了薄膜磁铁的磁化特性。 R-Fe-B类薄膜磁体可以在物理成膜或/和随后的热处理中加热至700℃至1200℃,从而生长晶粒并形成富含R元素的薄膜 晶界相。
摘要:
A method of manufacturing a rare earth permanent magnet comprises the steps of: forming a rare earth magnet by applying mechanical processing to a magnet block material, thereby damaging the surface of the magnet and causing a magnetic characteristic (BH)max of the magnet to deteriorate, followed by transforming a rare earth metal or an alloy thereof into fine particles or a vapor, and allowing the fine particles or vapor to diffuse and permeate the magnet, thereby improving the quality of the damaged magnet surface portion so that the magnetic characteristic (BH)max is recovered.
摘要:
A method of manufacturing a rare earth permanent magnet comprises the steps of: forming a rare earth magnet by applying mechanical processing to a magnet block material, thereby damaging the surface of the magnet and causing a magnetic characteristic (BH)max of the magnet to deteriorate, followed by transforming a rare earth metal or an alloy thereof into fine particles or a vapor, and allowing the fine particles or vapor to diffuse and permeate the magnet, thereby improving the quality of the damaged magnet surface portion so that the magnetic characteristic (BH)max is recovered.
摘要:
[Problem] In known methods, an improvement of the coercive force is realized by allowing the Dy metal or the like to present selectively in crystal grain boundary portions of a sintered magnet. However, since these are based on a physical film formation method, e.g., sputtering, through the use of a vacuum vessel, there is a mass productivity problem in the case where large amounts of magnet is treated. Furthermore, there is a magnet cost problem from the viewpoint that, for example, an expensive, high-purity Dy metal or the like must be used as a raw material for film formation. [Solving Means] A method for modifying grain boundaries of a Nd—Fe—B base magnet characterized by including the step of allowing an M metal component to diffuse and penetrate from a surface of a Nd—Fe—B base sintered magnet body having a Nd-rich crystal grain boundary phase surrounding principal Nd2Fe14B crystals to the grain boundary phase through a reduction treatment of a fluoride, an oxide, or a chloride of an M metal element (where M is Pr, Dy, Tb, or Ho).
摘要翻译:[问题]在已知的方法中,通过使Dy金属等选择性地存在于烧结磁体的晶界部中,可以实现矫顽力的提高。 然而,由于这些基于物理成膜方法,例如溅射,通过使用真空容器,在处理大量磁体的情况下存在批量生产率问题。 此外,从例如必须使用昂贵,高纯度的Dy金属等作为成膜原料的观点出现磁铁成本问题。 [解决方案]一种用于改变Nd-Fe-B基础磁体的晶界的方法,其特征在于包括以下步骤:允许M金属组分从具有 通过氟化物,氧化物或氯化物的还原处理将包围主要Nd 2 Fe 14 B的富Nd晶界相结晶到晶界相 M金属元素(其中M为Pr,Dy,Tb或Ho)。
摘要:
In known methods, an improvement of the coercive force is realized by allowing the Dy metal or the like to present selectively in crystal grain boundary portions of a sintered magnet. However, since these are based on a physical film formation method, e.g., sputtering, through the use of a vacuum vessel, there is a mass productivity problem when a large number of magnets are treated. Furthermore, there is a magnet cost problem from the viewpoint that, for example, an expensive, high-purity Dy metal or the like must be used as a raw material for film formation. The method for modifying grain boundaries of a Nd—Fe—B base magnet includes the step of allowing an M metal component to diffuse and penetrate from a surface of a Nd—Fe—B base sintered magnet body having a Nd-rich crystal grain boundary phase surrounding principal Nd2Fe14B crystals to the grain boundary phase through a reduction treatment of a fluoride, an oxide, or a chloride of an M metal element (where M is Pr, Dy, Tb, or Ho).
摘要翻译:在已知的方法中,通过使Dy金属等选择性地存在于烧结磁体的晶界部分中,可以实现矫顽力的提高。 然而,由于这些是基于物理成膜方法,例如溅射,通过使用真空容器,当大量的磁体被处理时,存在批量生产率问题。 此外,从例如必须使用昂贵,高纯度的Dy金属等作为成膜原料的观点出现磁铁成本问题。 Nd-Fe-B基磁体的晶界的修饰方法包括使M金属成分从具有富Nd晶界的Nd-Fe-B基烧结磁体的表面扩散并贯穿的步骤 通过还原处理M金属元素(其中M是Pr,Dy,Tb或Ho)的氟化物,氧化物或氯化物,使主要的Nd 2 Fe 14 B晶体相向晶界相。
摘要:
[Object] To provide a high-performance rare earth-based magnet exhibiting a high coercive force or a high residual magnetic flux density even when the content of a rare earth element such as Dy or the like which is scarce is reduced. [Construction] A rare earth-iron-boron based magnet includes a crystal grain boundary layer enriched in element M (M is at least one rare earth element selected from Pr, Dy, Tb, and Ho) by diffusion of the element M from the surface of the magnet, wherein the relation between the coercive force Hcj and the content of the element M in the whole of the magnet is represented by the following expression: Hcj≧1+0.2×M (wherein 0.05≦M≦10) wherein Hcj is the coercive force (unit: MA/m), and M is the content of the element M in the whole of the magnet (% by mass). Furthermore, the magnet satisfies the following expression: Br≧1.68−0.17×Hcj wherein Br is the residual magnetic flux density (unit: T).
摘要:
An apparatus for controlling stiffness of a vehicle body includes a slide member, a base member, a deformable member and an actuator. The slide member is disposed parallel to a direction of impact force acting on a first end of the slide member. The base member, which is disposed at a second end of the slide member, has a slit into which the slide member moves. The deformable member is disposed at the first end of the slide member. Both ends of the deformable member are connected to the base member and a cross section of the deformable member is substantially U-shaped. The actuator executes one of permitting the slide member to move into the slit and inhibiting the slide member from moving into the slit at a collision.
摘要:
Bubbles mixed in liquid crystal injected into a liquid crystal cell are pushed out through an outlet. The outlet has a space secured to a maximum limit by an extended sealing portion reaching the outer peripheral end surfaces of substrates, and a step with a color filter is formed. The pushed-out bubbles are surely trapped by the space of the outlet. In a replenishing port for replenishing liquid crystal, an introduction spacer having a height equal to that of the color filter is provided, and by a capillary phenomenon, liquid crystal for replenishment can be smoothly introduced into the liquid crystal cell.
摘要:
A rubbing direction (X) for each upper substrate of a tile panel constituting a liquid crystal panel unit is set along a horizontal direction (H) of the liquid crystal panel unit, a rubbing direction (Y) for each lower substrate of the tile panel is set along a vertical direction (V) thereof, and absorption axes (S) of polarizing plates and are allowed to coincide with the horizontal direction (H) of the liquid crystal panel unit. Moreover, in a set of four tile panels, the rubbing directions (X) and (Y) are made to differ from one another, thus viewing directions (Z) of high contrast are distributed into four directions, and turning directions (reference codes (R) and (L)) of liquid crystal molecules in the respective tile panels are arranged alternately in the horizontal direction (H) of the liquid crystal panel unit.