WO2021223436A1 - High-performance neodymium iron boron permanent magnet material and preparation method therefor - Google Patents

High-performance neodymium iron boron permanent magnet material and preparation method therefor Download PDF

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WO2021223436A1
WO2021223436A1 PCT/CN2020/134901 CN2020134901W WO2021223436A1 WO 2021223436 A1 WO2021223436 A1 WO 2021223436A1 CN 2020134901 W CN2020134901 W CN 2020134901W WO 2021223436 A1 WO2021223436 A1 WO 2021223436A1
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rare earth
heavy rare
powder
iron boron
neodymium iron
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PCT/CN2020/134901
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French (fr)
Chinese (zh)
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舒泽腾
郑波
郭帅
陈仁杰
丁广飞
闫阿儒
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中国科学院宁波材料技术与工程研究所
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/047Alloys characterised by their composition
    • H01F1/053Alloys characterised by their composition containing rare earth metals
    • H01F1/055Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
    • H01F1/057Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B
    • H01F1/0571Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes
    • H01F1/0575Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes pressed, sintered or bonded together
    • H01F1/0576Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes pressed, sintered or bonded together pressed, e.g. hot working
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/047Alloys characterised by their composition
    • H01F1/053Alloys characterised by their composition containing rare earth metals
    • H01F1/055Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5
    • H01F1/057Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B
    • H01F1/0571Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes
    • H01F1/0575Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes pressed, sintered or bonded together
    • H01F1/0577Alloys characterised by their composition containing rare earth metals and magnetic transition metals, e.g. SmCo5 and IIIa elements, e.g. Nd2Fe14B in the form of particles, e.g. rapid quenched powders or ribbon flakes pressed, sintered or bonded together sintered
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F1/00Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties
    • H01F1/01Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials
    • H01F1/03Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity
    • H01F1/032Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials
    • H01F1/04Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys
    • H01F1/06Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys in the form of particles, e.g. powder
    • H01F1/08Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys in the form of particles, e.g. powder pressed, sintered, or bound together
    • H01F1/086Magnets or magnetic bodies characterised by the magnetic materials therefor; Selection of materials for their magnetic properties of inorganic materials characterised by their coercivity of hard-magnetic materials metals or alloys in the form of particles, e.g. powder pressed, sintered, or bound together sintered
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/02Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
    • H01F41/0253Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing permanent magnets
    • H01F41/0266Moulding; Pressing
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F41/00Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
    • H01F41/02Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
    • H01F41/0253Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing permanent magnets
    • H01F41/0273Imparting anisotropy

Definitions

  • the invention relates to the technical field of magnetic materials, in particular to a neodymium iron boron permanent magnet material and a preparation method thereof.
  • Sintered NdFeB permanent magnet material is currently the magnetic material with the highest comprehensive magnetic performance among permanent magnet materials. Because neodymium iron boron magnets have high remanence Br and maximum magnetic energy product (BH) max , they can reduce the volume and cost of magnetic devices. Therefore, this material is widely used in electronic information, medical equipment, and new energy vehicles. In the field of other magnetic devices, it has a wide range of application prospects.
  • BH maximum magnetic energy product
  • the anti-ferromagnetic interaction between the irons leads to a significant reduction in the remanence of the magnet; some researchers use the method of grain boundary diffusion to ensure that the remanence of the magnet does not drop or drop slightly, that is, a large amount of metal elements Tb and Dy are passed Coating or magnetron sputtering, coating on the surface of the magnet, and finally through heat treatment to prepare a neodymium iron boron magnet. Although this method can ensure that the remanence Br of the magnet does not drop or drop slightly, it has strict requirements on the size of the neodymium iron boron magnet. The thickness direction of the magnet orientation generally does not exceed 6mm. Therefore, the research on reducing the amount of heavy rare earths while maintaining high coercivity and high remanence has attracted wide attention.
  • the technical problem solved by the present invention is to provide a neodymium iron boron permanent magnet material.
  • the neodymium iron boron permanent magnet material provided in this application can reduce the use of heavy rare earth elements and ensure that the remanence of the neodymium iron boron magnet does not drop or slightly drops. , The coercivity has been significantly improved.
  • the present application provides a neodymium iron boron permanent magnet material, which is prepared from an anisotropic magnet as shown in formula (I) and heavy rare earth as shown in formula (II).
  • the mass ratio of the anisotropic magnet to the total amount of the heavy rare earth is 0.1-5wt%;
  • M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
  • the weight ratio of the heavy rare earth in the total amount of the anisotropic magnet and the heavy rare earth is 1 wt% to 2 wt%.
  • the M is selected from Co, Al, Cu, Zr and Ga.
  • the neodymium iron boron permanent magnet material includes a main phase structure and a shell structure around the main phase structure, the main phase structure is (Nd, Pr) 2 Fe 14 B, and the shell structure is (Tb ,Nd) 2 Fe 14 B.
  • the application also provides a method for preparing the neodymium iron boron permanent magnet material, which includes the following steps:
  • the mixed magnetic powder is oriented, pressed, sintered and tempered in sequence to obtain a neodymium iron boron permanent magnet material
  • M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
  • the anisotropic magnet powder is prepared by a hydrogen breaking-jet milling process, and the particle size of the anisotropic magnet powder is 1.5-3.0 ⁇ m.
  • the preparation method of the anisotropic magnet powder is specifically:
  • the alloy flakes are crushed by hydrogen cracking and jet mill to obtain anisotropic magnet powder.
  • the method for preparing the heavy rare earth powder is specifically:
  • the master alloy is pulverized through a hydrogen breaking-jet milling process or a ball milling process to obtain heavy rare earth powder; the particle size of the heavy rare earth powder is 0.1 ⁇ m-2 ⁇ m.
  • the orientation pressing type is specifically:
  • the mixed magnetic powder is press-formed at 2.3-2.5T, and then statically pressed at 150-200 MPa to obtain a blank magnet.
  • the sintering temperature is 1060°C to 1075°C
  • the sintering time is 2 to 4 hours
  • the tempering treatment includes one-stage tempering and two-stage tempering in a vacuum environment or a protective atmosphere.
  • the temperature of the first-stage tempering is 850-900°C
  • the time of the first-stage tempering is 1h-3h
  • the temperature of the second-stage tempering is 480-550°C
  • the time of the second-stage tempering It is 1h ⁇ 3h.
  • This application provides a neodymium iron boron permanent magnet material, which is prepared from an anisotropic magnet (Nd, Pr) x Fe (100-xyz) B y M z and heavy rare earth Tb a Fe b Al 100-ab ;
  • the Tb and Al elements in the heavy rare earth in the NdFeB permanent magnet material can increase the coercivity, and the Tb element can form the Tb2Fe4B phase with high anisotropy field, which can greatly increase the coercivity Hcj.
  • Al is in the rich NdPr grain boundary. In this case, it can lubricate the grain boundary and increase the coercive force Hcj.
  • the Fe element itself has a higher saturation magnetic polarization and maintains a high remanence Br; therefore, the neodymium iron boron permanent magnet material provided in this application is added with heavy rare earth The components and the amount of addition are controlled, so that the coercivity of the neodymium iron boron permanent magnet material can be significantly improved without the remanence of the neodymium iron boron permanent magnet material being reduced or slightly reduced.
  • Figure 1 is a scanning electron micrograph of an anisotropic neodymium iron boron permanent magnet material [(NdPr) 29.5 Cu 0.2 Al 0.1 Zr 0.2 Co 0.5 Ga 0.1 Fe bal. B 0.9 ];
  • Figure 2 is a scanning electron micrograph of the neodymium iron boron permanent magnet material obtained in Example 1;
  • Figure 3 is a scanning electron micrograph of the neodymium iron boron permanent magnet material obtained in Example 2;
  • Example 4 is a scanning electron micrograph of the neodymium iron boron permanent magnet material obtained in Example 3;
  • FIG. 5 is a scanning electron microscope photograph of the neodymium iron boron permanent magnet material obtained in Comparative Example 1.
  • FIG. 5 is a scanning electron microscope photograph of the neodymium iron boron permanent magnet material obtained in Comparative Example 1.
  • this application provides a neodymium iron boron permanent magnet material, which on the basis of reducing the amount of heavy rare earth used, does not reduce the remanence. Or in the case of a slight drop, the coercivity of the neodymium iron boron permanent magnet material can be significantly improved.
  • the embodiment of the present invention discloses a neodymium iron boron permanent magnet material, which is prepared from an anisotropic magnet as shown in formula (I) and a heavy rare earth as shown in formula (II). The mass ratio of the anisotropic magnet and the total amount of the heavy rare earth is ⁇ 0.1wt% and ⁇ 5.0wt%;
  • M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
  • the anisotropic magnet (Nd, Pr) x Fe (100-xyz) B y M z has a lower (Nd, Pr) content and a lower B content, so It can maintain high remanence Br, and at the same time there is an abundant NdPr grain boundary phase at the grain boundary of the magnet.
  • the M is selected from one or more of Co, Al, Cu, Zr, Ti, Ni, and Ga. In a specific embodiment, the M is selected from Co, Al, Cu, Zr and Ga, and the M is selected In the case of multiple alloying elements, the content of each element can be adjusted, as long as the total range is 0 to 2.5 ( ⁇ 0).
  • Nd, Pr in this application means one or two of Nd and Pr, and its content can be 28.6wt%, 28.7wt%, 28.8wt%, 28.9wt%, 29.0wt%, 29.1wt%, 29.2 wt%, 29.3 wt%, 29.4 wt%, 29.5 wt%, 29.6% wt, or 29.7% wt.
  • the content of B is 0.86wt%, 0.87wt%, 0.88wt%, 0.89wt% or 0.90wt%.
  • the content of M is 0.2 to 2.3 wt%, and in a specific embodiment, the content of M is 1.0 to 1.8 wt%.
  • Tb and Al are added to the heavy rare earth component Tb a Fe b Al 100-ab to increase the coercivity.
  • the Tb element can form a phase of Tb2Fe4B with a high anisotropy field, which can greatly increase the coercivity Hcj. In the case of abundant NdPr grain boundaries, it can lubricate the grain boundaries and increase the coercivity Hcj.
  • the Fe element itself has a higher saturation magnetic polarization and maintains a high remanence Br.
  • the heavy rare earth accounts for 0.1 to 5 wt% of the total amount of the anisotropic magnet and the heavy rare earth; in a specific embodiment, the heavy rare earth accounts for the various directions 1 to 2 wt% of the total amount of the heterogeneous magnet and the heavy rare earth; less than 0.1 wt%, the coercive force increasing effect is not obvious, and more than 5 wt%, the remanence Br decreases too much.
  • the application also provides a preparation method of the above-mentioned neodymium iron boron permanent magnet material, which includes the following steps:
  • the mixed magnetic powder is oriented, pressed, sintered and tempered in sequence to obtain a neodymium iron boron permanent magnet material
  • M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
  • the present application first mixes the anisotropic magnet powder and the heavy rare earth powder to obtain the mixed powder; the mixing time is 1 to 3 hours. Before the two are mixed, the anisotropic magnet powder and the heavy rare earth powder are prepared separately; the preparation method of the anisotropic magnet powder is specifically as follows:
  • the alloy flakes are crushed by hydrogen cracking and jet mill to obtain anisotropic magnet powder.
  • the preparation method of the heavy rare earth powder is specifically as follows:
  • the master alloy is pulverized through a hydrogen breaking-jet milling process or a ball milling process to obtain heavy rare earth powder.
  • the anisotropic magnet powder has a particle size of 1.5 to 3.0 m, and the heavy rare earth powder has a particle size of 0.1 to 2.0 m.
  • the mixed magnetic powder obtained above is sequentially subjected to orientation pressing, sintering and tempering, thereby obtaining a neodymium iron boron permanent magnet material; in the above process, the orientation pressing, sintering and tempering are based Technical and technological means well known to those skilled in the art, this application does not impose special restrictions on their technological operations.
  • the orientation molding is specifically to press and mold the mixed magnetic powder at 2.3-2.5T, and then statically press at 150-200 MPa to obtain a blank magnet.
  • the sintering temperature is 1060-1075°C, and the time is 2-4h.
  • the first-stage tempering and the second-stage tempering are sequentially performed in the vacuum environment or protective atmosphere of the tempering treatment, the temperature of the first-stage tempering is 850-900°C, and the time of the first-stage tempering is 1h-3h
  • the temperature of the secondary tempering is 480°C to 550°C, and the time of the secondary tempering is 1h-3h.
  • the neodymium iron boron permanent magnet material provided by the present application includes a main phase structure and a shell structure uniformly distributed around the main phase structure.
  • the composition of the shell structure is (Tb, Nd) 2 Fe 14 B.
  • the main phase structure It is (Nd, Pr) 2 Fe 14 B.
  • the preparation method of the high-performance neodymium iron boron permanent magnet material provided by the present invention can significantly increase the coercivity of the neodymium iron boron permanent magnet material while not affecting the neodymium iron boron permanent magnet under the condition that the remanence is not reduced or slightly reduced.
  • the magnetic properties of the material are suitable for mass production of large-size blanks; the preparation method of the high-performance neodymium iron boron permanent magnet material provided by the present invention can effectively reduce the amount of heavy rare earth used.
  • the preparation method of the high-performance neodymium iron boron permanent magnet material provided by the invention is simple and easy to implement and can be industrialized.
  • the chemical formula of anisotropic magnetic powder is (NdPr) 29.5 Cu 0.2 Al 0.1 Zr 0.2 Co 0.5 Ga 0.1 Fe bal. B 0.9 , the chemical formula of heavy rare earth powder is Tb 60 Fe 38 Al 2 , and the doping amount of heavy rare earth powder is mixed magnetic powder 1%;
  • the prepared NdFeB permanent magnet material was tested, and the results are shown in Table 1. From Table 1, the coercivity Hcj of the NdFeB permanent magnet material is higher than that of the permanent magnet material without heavy rare earth magnetic powder. After 3.18kOe, there is almost no change in the remanence Br.
  • This preparation method is basically the same as the preparation method of Example 1, except that the doping amount of the heavy rare earth powder is 2% of the mixed magnetic powder.
  • the prepared NdFeB permanent magnet material was tested, and the results are shown in Table 1. From Table 1, the coercivity Hcj of the NdFeB permanent magnet material is higher than that of the permanent magnet material without heavy rare earth magnetic powder. When the output is 6.54kOe, the remanence Br is reduced by 0.19kGs.
  • This preparation method is basically the same as the preparation method of Example 1, except that the doping amount of the heavy rare earth powder is 4% of the mixed magnetic powder.
  • the prepared NdFeB permanent magnet material was tested, and the results are shown in Table 1. From Table 1, the coercivity Hcj of the NdFeB permanent magnet material is higher than that of the permanent magnet material without heavy rare earth magnetic powder. Out of 10.03kOe, the remanence Br is reduced by 1.18kGs.
  • This preparation method is basically the same as the preparation method of Example 1, except that the doping amount of the heavy rare earth powder is 6% of the mixed magnetic powder.
  • the prepared neodymium iron boron permanent magnet material was tested, and the Br of the magnet prepared in this comparative example was 12.42 KGs, and the Hcj was 28.56 KOe. It can be seen from Fig. 5 that the core of the core-shell structure in the main phase grains is further reduced, which indicates that the heavy rare earth elements are doped too much, which makes the remanence decrease too much.

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Abstract

A neodymium iron boron permanent magnet material and a preparation method therefor. The neodymium iron boron permanent magnet material is prepared by an anisotropic magnet as shown in formula (Nd, Pr)x <sb />Fe(100-x-y-z)ByMz and heavy rare earth as shown in formula TbaFebAl100-a-b, and the mass ratio of the heavy rare earth to the total amount of the anisotropic magnet and the heavy rare earth is 0.1-5 wt%. On the basis of reducing the use amount of heavy rare earth elements, the neodymium iron boron permanent magnet material can ensure that the coercive force of a neodymium iron boron magnet is obviously improved while the residual magnetism of the neodymium iron boron magnet is not reduced or slightly reduced, thus greatly reducing production costs.

Description

一种高性能钕铁硼永磁材料及其制备方法High-performance neodymium iron boron permanent magnet material and preparation method thereof
本申请要求于2020年05月08日提交中国专利局、申请号为202010382427.8、发明名称为“一种高性能钕铁硼永磁材料及其制备方法”的中国专利申请的优先权,其全部内容通过引用结合在本申请中。This application claims the priority of a Chinese patent application filed with the Chinese Patent Office on May 8, 2020, the application number is 202010382427.8, and the invention title is "a high-performance neodymium iron boron permanent magnet material and its preparation method", and its entire content Incorporated in this application by reference.
技术领域Technical field
本发明涉及磁性材料技术领域,尤其涉及一种钕铁硼永磁材料及其制备方法。The invention relates to the technical field of magnetic materials, in particular to a neodymium iron boron permanent magnet material and a preparation method thereof.
背景技术Background technique
烧结钕铁硼永磁材料是目前永磁材料中综合磁性能最高的磁性材料。由于钕铁硼磁体具有高的剩磁Br及最大的磁能积(BH) max,能够减少磁性器件的体积及降低器件的成本,因此这种材料大量的应用在电子信息、医疗设备、新能源汽车等磁性器件领域,具有广泛的应用前景。 Sintered NdFeB permanent magnet material is currently the magnetic material with the highest comprehensive magnetic performance among permanent magnet materials. Because neodymium iron boron magnets have high remanence Br and maximum magnetic energy product (BH) max , they can reduce the volume and cost of magnetic devices. Therefore, this material is widely used in electronic information, medical equipment, and new energy vehicles. In the field of other magnetic devices, it has a wide range of application prospects.
随着工业化快速的发展,磁性器件的小型化需求对钕铁硼磁体提出了更高的要求,既要大幅度提高剩磁Br,又要提升矫顽力Hcj。目前,在工业上广泛采用添加重稀土Tb、Dy等元素提高各向异性场,从而达到提高磁体矫顽力Hcj的目的,但是由于重稀土Tb、Dy的成本较高,同时重稀土元素会与铁之间产生反铁磁作用导致磁体的剩磁大幅度明显降低;还有部分研究者采用晶界扩散的方法保证磁体剩磁不降或微降,即将大量的金属元素Tb,Dy元素,通过涂覆或磁控溅射,涂覆在磁体表面,最后经过热处理制备得到钕铁硼磁体,该方法虽然可以保证磁体剩磁Br的不降或微降,但是对钕铁硼磁体尺寸要求严格,磁体取向厚度方向一般不超过6mm。因而,在降低重稀土用量,同时保持高矫顽力高剩磁的研究受到广泛的关注。With the rapid development of industrialization, the demand for miniaturization of magnetic devices puts forward higher requirements on neodymium iron boron magnets, not only to greatly increase the remanence Br, but also to increase the coercive force Hcj. At present, the addition of heavy rare earth Tb, Dy and other elements is widely used in industry to increase the anisotropy field, so as to achieve the purpose of increasing the coercive force Hcj of the magnet. The anti-ferromagnetic interaction between the irons leads to a significant reduction in the remanence of the magnet; some researchers use the method of grain boundary diffusion to ensure that the remanence of the magnet does not drop or drop slightly, that is, a large amount of metal elements Tb and Dy are passed Coating or magnetron sputtering, coating on the surface of the magnet, and finally through heat treatment to prepare a neodymium iron boron magnet. Although this method can ensure that the remanence Br of the magnet does not drop or drop slightly, it has strict requirements on the size of the neodymium iron boron magnet. The thickness direction of the magnet orientation generally does not exceed 6mm. Therefore, the research on reducing the amount of heavy rare earths while maintaining high coercivity and high remanence has attracted wide attention.
发明内容Summary of the invention
本发明解决的技术问题在于提供一种钕铁硼永磁材料,本申请提供的钕铁硼永磁材料能够降低重稀土元素的使用,保证钕铁硼磁体剩磁不降或微降的情况下,矫顽力得到明显的提升。The technical problem solved by the present invention is to provide a neodymium iron boron permanent magnet material. The neodymium iron boron permanent magnet material provided in this application can reduce the use of heavy rare earth elements and ensure that the remanence of the neodymium iron boron magnet does not drop or slightly drops. , The coercivity has been significantly improved.
有鉴于此,本申请提供了一种钕铁硼永磁材料,由如式(Ⅰ)所示的各向异性磁体和如式(Ⅱ)所示的重稀土制备得到,所述重稀土占所述各向异性磁体和所述重稀土总量的质量比例为0.1~5wt%;In view of this, the present application provides a neodymium iron boron permanent magnet material, which is prepared from an anisotropic magnet as shown in formula (I) and heavy rare earth as shown in formula (II). The mass ratio of the anisotropic magnet to the total amount of the heavy rare earth is 0.1-5wt%;
(Nd,Pr) xFe (100-x-y-z)B yM z   (Ⅰ); (Nd,Pr) x Fe (100-xyz) B y M z (Ⅰ);
Tb aFe bAl 100-a-b    (Ⅱ); Tb a Fe b Al 100-ab (Ⅱ);
其中,28.6wt%≤x≤29.5wt%,0.85wt%≤y≤0.9wt%,0<z≤2.5wt%,M选自Co、Al、Cu、Zr、Ti、Ni和Ga中的一种或多种;Among them, 28.6wt%≤x≤29.5wt%, 0.85wt%≤y≤0.9wt%, 0<z≤2.5wt%, M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
60wt%≤a≤92wt%,6wt%≤b≤38wt%,a+b=100wt%。60wt%≤a≤92wt%, 6wt%≤b≤38wt%, a+b=100wt%.
优选的,所述重稀土占所述各向异性磁体和所述重稀土总量的质量比例为1wt%~2wt%。Preferably, the weight ratio of the heavy rare earth in the total amount of the anisotropic magnet and the heavy rare earth is 1 wt% to 2 wt%.
优选的,所述M选自Co、Al、Cu、Zr和Ga。Preferably, the M is selected from Co, Al, Cu, Zr and Ga.
优选的,所述钕铁硼永磁材料包括主相结构和位于主相结构周围的壳层结构,所述主相结构为(Nd,Pr) 2Fe 14B,所述壳层结构为(Tb,Nd) 2Fe 14B。 Preferably, the neodymium iron boron permanent magnet material includes a main phase structure and a shell structure around the main phase structure, the main phase structure is (Nd, Pr) 2 Fe 14 B, and the shell structure is (Tb ,Nd) 2 Fe 14 B.
本申请还提供了所述的钕铁硼永磁材料的制备方法,包括以下步骤:The application also provides a method for preparing the neodymium iron boron permanent magnet material, which includes the following steps:
A)将如式(Ⅰ)所示的各向异性磁体粉末和如式(Ⅱ)所示的重稀土粉末混合,得到混合磁粉,所述混合磁粉中所述重稀土粉末的质量比例为0.1~5wt%;A) Mixing the anisotropic magnet powder as shown in formula (I) and the heavy rare earth powder as shown in formula (II) to obtain mixed magnetic powder. The mass ratio of the heavy rare earth powder in the mixed magnetic powder is 0.1~ 5wt%;
B)将所述混合磁粉依次进行取向压型、烧结和回火,得到钕铁硼永磁材料;B) The mixed magnetic powder is oriented, pressed, sintered and tempered in sequence to obtain a neodymium iron boron permanent magnet material;
(Nd,Pr) xFe (100-x-y-z)B yM z    (Ⅰ); (Nd,Pr) x Fe (100-xyz) B y M z (Ⅰ);
Tb aFe bAl 100-a-b     (Ⅱ); Tb a Fe b Al 100-ab (Ⅱ);
其中,28.6wt%≤x≤29.5wt%,0.85wt%≤y≤0.9wt%,0<z≤2.5wt%,M选自Co、Al、Cu、Zr、Ti、Ni和Ga中的一种或多种;Among them, 28.6wt%≤x≤29.5wt%, 0.85wt%≤y≤0.9wt%, 0<z≤2.5wt%, M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
60wt%≤a≤92wt%,6wt%≤b≤38wt%,a+b=100wt%。60wt%≤a≤92wt%, 6wt%≤b≤38wt%, a+b=100wt%.
优选的,所述各向异性磁体粉末通过氢破-气流磨工艺制备得到,所述各向异性磁体粉末的粒径为1.5~3.0μm。Preferably, the anisotropic magnet powder is prepared by a hydrogen breaking-jet milling process, and the particle size of the anisotropic magnet powder is 1.5-3.0 μm.
优选的,所述各向异性磁体粉末的制备方法具体为:Preferably, the preparation method of the anisotropic magnet powder is specifically:
按照式(Ⅰ)中各向异性磁体粉末中各元素的比例配料;According to formula (I), the proportion of each element in the anisotropic magnet powder;
将配好的原料混合在惰性气氛下进行熔炼,得到母合金;Mix the prepared raw materials in an inert atmosphere for smelting to obtain a master alloy;
将所述母合金速凝制成合金片;Rapid solidification of the master alloy into alloy flakes;
将所述合金片通过氢破、气流磨进行粉碎,得到各向异性磁体粉末。The alloy flakes are crushed by hydrogen cracking and jet mill to obtain anisotropic magnet powder.
优选的,所述重稀土粉末的制备方法具体为:Preferably, the method for preparing the heavy rare earth powder is specifically:
按照式(Ⅱ)中各元素的比例配料;Ingredients according to the proportion of each element in formula (II);
将配好的原料混合并在惰性气氛下进行熔炼,得到重稀土母合金;Mix the prepared raw materials and smelt in an inert atmosphere to obtain a heavy rare earth master alloy;
将所述母合金通过氢破-气流磨工艺或者球磨工艺进行粉碎,得到重稀土粉末;所述的重稀土粉末的粒径为0.1μm~2μm。The master alloy is pulverized through a hydrogen breaking-jet milling process or a ball milling process to obtain heavy rare earth powder; the particle size of the heavy rare earth powder is 0.1 μm-2 μm.
优选的,所述取向压型具体为:Preferably, the orientation pressing type is specifically:
将所述混合磁粉在2.3~2.5T压制成型,再于150~200MPa静压,得到毛坯磁体。The mixed magnetic powder is press-formed at 2.3-2.5T, and then statically pressed at 150-200 MPa to obtain a blank magnet.
优选的,所述烧结的温度为1060℃~1075℃,所述烧结的时间为2~4h,所述回火处理包括真空环境或保护气氛中依次进行的一级回火和二级回火,所述一级回火的温度为850~900℃,所述一级回火的时间为1h~3h,所述二级回火的温度为480℃~550℃,所述二级回火的时间为1h~3h。Preferably, the sintering temperature is 1060°C to 1075°C, the sintering time is 2 to 4 hours, and the tempering treatment includes one-stage tempering and two-stage tempering in a vacuum environment or a protective atmosphere. The temperature of the first-stage tempering is 850-900°C, the time of the first-stage tempering is 1h-3h, the temperature of the second-stage tempering is 480-550°C, and the time of the second-stage tempering It is 1h~3h.
本申请提供了一种钕铁硼永磁材料,其由各向异性磁体(Nd,Pr) xFe (100-x-y-z)B yM z和重稀土Tb aFe bAl 100-a-b制备得到;在钕铁硼永磁材料中重稀土中Tb和Al元素可提高矫顽力,Tb元素能够形成高各向异性场的Tb2Fe4B相,更够大幅度提升矫顽力Hcj,Al在富足NdPr晶界的情况下,能够润滑晶界边界,提升矫顽力Hcj,Fe元素本身有较高的饱和磁极化强度,保持高剩磁Br;因此,本申请中提供的钕铁硼永磁材料通过加入重稀土组分,且控制其加入量,使得钕铁硼永磁材料在剩磁不降低或微降的情况下,可以明显提升钕铁硼永磁材料的矫顽力。 This application provides a neodymium iron boron permanent magnet material, which is prepared from an anisotropic magnet (Nd, Pr) x Fe (100-xyz) B y M z and heavy rare earth Tb a Fe b Al 100-ab ; The Tb and Al elements in the heavy rare earth in the NdFeB permanent magnet material can increase the coercivity, and the Tb element can form the Tb2Fe4B phase with high anisotropy field, which can greatly increase the coercivity Hcj. Al is in the rich NdPr grain boundary. In this case, it can lubricate the grain boundary and increase the coercive force Hcj. The Fe element itself has a higher saturation magnetic polarization and maintains a high remanence Br; therefore, the neodymium iron boron permanent magnet material provided in this application is added with heavy rare earth The components and the amount of addition are controlled, so that the coercivity of the neodymium iron boron permanent magnet material can be significantly improved without the remanence of the neodymium iron boron permanent magnet material being reduced or slightly reduced.
附图说明Description of the drawings
图1为各向异性钕铁硼永磁材料[(NdPr) 29.5Cu 0.2Al 0.1Zr 0.2Co 0.5Ga 0.1Fe bal.B 0.9]的扫描电镜照片; Figure 1 is a scanning electron micrograph of an anisotropic neodymium iron boron permanent magnet material [(NdPr) 29.5 Cu 0.2 Al 0.1 Zr 0.2 Co 0.5 Ga 0.1 Fe bal. B 0.9 ];
图2为实施例1得到的钕铁硼永磁材料的扫描电镜照片;Figure 2 is a scanning electron micrograph of the neodymium iron boron permanent magnet material obtained in Example 1;
图3为实施例2得到的钕铁硼永磁材料的扫描电镜照片;Figure 3 is a scanning electron micrograph of the neodymium iron boron permanent magnet material obtained in Example 2;
图4为实施例3得到的钕铁硼永磁材料的扫描电镜照片;4 is a scanning electron micrograph of the neodymium iron boron permanent magnet material obtained in Example 3;
图5为对比例1得到的钕铁硼永磁材料的扫描电镜照片。FIG. 5 is a scanning electron microscope photograph of the neodymium iron boron permanent magnet material obtained in Comparative Example 1. FIG.
具体实施方式Detailed ways
为了进一步理解本发明,下面结合实施例对本发明优选实施方案进行描述,但是应当理解,这些描述只是为进一步说明本发明的特征和优点,而不是 对本发明权利要求的限制。In order to further understand the present invention, the preferred embodiments of the present invention are described below in conjunction with examples, but it should be understood that these descriptions are only for further illustrating the features and advantages of the present invention, rather than limiting the claims of the present invention.
鉴于现有技术中钕铁硼磁体矫顽力和剩磁不平衡的问题,本申请提供了一种钕铁硼永磁材料,其在降低重稀土的使用量的基础上,在剩磁不降或微降的情况下,可以明显的提升钕铁硼永磁材料的矫顽力。具体的,本发明实施例公开了一种钕铁硼永磁材料,由如式(Ⅰ)所示的各向异性磁体和如式(Ⅱ)所示的重稀土制备得到,所述重稀土占所述各向异性磁体和所述重稀土总量的质量比例≥0.1wt%且≤5.0wt%;In view of the imbalance of coercivity and remanence of neodymium iron boron magnets in the prior art, this application provides a neodymium iron boron permanent magnet material, which on the basis of reducing the amount of heavy rare earth used, does not reduce the remanence. Or in the case of a slight drop, the coercivity of the neodymium iron boron permanent magnet material can be significantly improved. Specifically, the embodiment of the present invention discloses a neodymium iron boron permanent magnet material, which is prepared from an anisotropic magnet as shown in formula (I) and a heavy rare earth as shown in formula (II). The mass ratio of the anisotropic magnet and the total amount of the heavy rare earth is ≥0.1wt% and ≤5.0wt%;
(Nd,Pr) xFe (100-x-y-z)B yM z     (Ⅰ); (Nd,Pr) x Fe (100-xyz) B y M z (Ⅰ);
Tb aFe bAl 100-a-b     (Ⅱ); Tb a Fe b Al 100-ab (Ⅱ);
其中,28.6wt%≤x≤29.5wt%,0.85wt%≤y≤0.9wt%,0<z≤2.5wt%,M选自Co、Al、Cu、Zr、Ti、Ni和Ga中的一种或多种;Among them, 28.6wt%≤x≤29.5wt%, 0.85wt%≤y≤0.9wt%, 0<z≤2.5wt%, M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
60wt%≤a≤92wt%,6wt%≤b≤38wt%,a+b=100wt%。60wt%≤a≤92wt%, 6wt%≤b≤38wt%, a+b=100wt%.
在本申请所述钕铁硼永磁材料中,各向异性磁体(Nd,Pr) xFe (100-x-y-z)B yM z中(Nd,Pr)含量较低,B的含量较低,如此可以保持高剩磁Br,同时在磁体晶界处有富足NdPr晶界相。所述M选自Co、Al、Cu、Zr、Ti、Ni和Ga中的一种或多种,在具体实施例中,所述M选自Co、Al、Cu、Zr和Ga,在M选择多种合金元素的情况下,每种元素的含量可进行调整,只要总和的范围为0~2.5(≠0)即可。(Nd,Pr)在本申请中表示Nd和Pr中的一种或两种,其含量可以为28.6wt%、28.7wt%、28.8wt%、28.9wt%、29.0wt%、29.1wt%、29.2wt%、29.3wt%、29.4wt%、29.5wt%、29.6wt%或29.7wt%。B的含量为0.86wt%、0.87wt%、0.88wt%、0.89wt%或0.90wt%。所述M的含量为0.2~2.3wt%,在具体实施例中,所述M的含量为1.0~1.8wt%。 Among the neodymium iron boron permanent magnet materials described in this application, the anisotropic magnet (Nd, Pr) x Fe (100-xyz) B y M z has a lower (Nd, Pr) content and a lower B content, so It can maintain high remanence Br, and at the same time there is an abundant NdPr grain boundary phase at the grain boundary of the magnet. The M is selected from one or more of Co, Al, Cu, Zr, Ti, Ni, and Ga. In a specific embodiment, the M is selected from Co, Al, Cu, Zr and Ga, and the M is selected In the case of multiple alloying elements, the content of each element can be adjusted, as long as the total range is 0 to 2.5 (≠0). (Nd, Pr) in this application means one or two of Nd and Pr, and its content can be 28.6wt%, 28.7wt%, 28.8wt%, 28.9wt%, 29.0wt%, 29.1wt%, 29.2 wt%, 29.3 wt%, 29.4 wt%, 29.5 wt%, 29.6% wt, or 29.7% wt. The content of B is 0.86wt%, 0.87wt%, 0.88wt%, 0.89wt% or 0.90wt%. The content of M is 0.2 to 2.3 wt%, and in a specific embodiment, the content of M is 1.0 to 1.8 wt%.
重稀土成分Tb aFe bAl 100-a-b中加入Tb、Al元素是为了提升矫顽力,Tb元素能够形成高各向异性场的Tb2Fe4B这种相,能够大幅度提升矫顽力Hcj,Al在富足NdPr晶界的情况下,能够润滑晶界边界,提升矫顽力Hcj,Fe元素本身有较高的饱和磁极化强度,保持高剩磁Br。 Tb and Al are added to the heavy rare earth component Tb a Fe b Al 100-ab to increase the coercivity. The Tb element can form a phase of Tb2Fe4B with a high anisotropy field, which can greatly increase the coercivity Hcj. In the case of abundant NdPr grain boundaries, it can lubricate the grain boundaries and increase the coercivity Hcj. The Fe element itself has a higher saturation magnetic polarization and maintains a high remanence Br.
在所述钕铁硼永磁材料中,所述重稀土占所述各向异性磁体和所述重稀土总量的0.1~5wt%;在具体实施例中,所述重稀土占所述各向异性磁体和所述重稀土总量的1~2wt%;低于0.1wt%则矫顽力增长效果不明显,高于5wt%则 剩磁Br降低过多。In the neodymium iron boron permanent magnet material, the heavy rare earth accounts for 0.1 to 5 wt% of the total amount of the anisotropic magnet and the heavy rare earth; in a specific embodiment, the heavy rare earth accounts for the various directions 1 to 2 wt% of the total amount of the heterogeneous magnet and the heavy rare earth; less than 0.1 wt%, the coercive force increasing effect is not obvious, and more than 5 wt%, the remanence Br decreases too much.
本申请还提供了上述钕铁硼永磁材料的制备方法,包括以下步骤:The application also provides a preparation method of the above-mentioned neodymium iron boron permanent magnet material, which includes the following steps:
A)将如式(Ⅰ)所示的各向异性磁体粉末和如式(Ⅱ)所示的重稀土粉末混合,得到混合磁粉,所述混合磁粉中所述重稀土粉末的质量比例≥0.1wt%且≤5.0wt%;A) Mix the anisotropic magnet powder as shown in formula (I) and the heavy rare earth powder as shown in formula (II) to obtain mixed magnetic powder, and the mass ratio of the heavy rare earth powder in the mixed magnetic powder is ≥0.1wt % And ≤5.0wt%;
B)将所述混合磁粉依次进行取向压型、烧结和回火,得到钕铁硼永磁材料;B) The mixed magnetic powder is oriented, pressed, sintered and tempered in sequence to obtain a neodymium iron boron permanent magnet material;
(Nd,Pr) xFe (100-x-y-z)B yM z    (Ⅰ); (Nd,Pr) x Fe (100-xyz) B y M z (Ⅰ);
Tb aFe bAl 100-a-b    (Ⅱ) Tb a Fe b Al 100-ab (Ⅱ)
其中,28.6wt%≤x≤29.5wt%,0.85wt%≤y≤0.9wt%,0<z≤2.5wt%,M选自Co、Al、Cu、Zr、Ti、Ni和Ga中的一种或多种;Among them, 28.6wt%≤x≤29.5wt%, 0.85wt%≤y≤0.9wt%, 0<z≤2.5wt%, M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
60wt%≤a≤92wt%,6wt%≤b≤38wt%,a+b=100wt%。60wt%≤a≤92wt%, 6wt%≤b≤38wt%, a+b=100wt%.
在上述制备过程中,本申请首先将各向异性磁体粉末和重稀土粉末混合,即得到混合粉;所述混合的时间为1~3h。在两者混合之前,首先分别制备各向异性磁体粉末和重稀土粉末;所述各向异型磁体粉末的制备方法具体为:In the above preparation process, the present application first mixes the anisotropic magnet powder and the heavy rare earth powder to obtain the mixed powder; the mixing time is 1 to 3 hours. Before the two are mixed, the anisotropic magnet powder and the heavy rare earth powder are prepared separately; the preparation method of the anisotropic magnet powder is specifically as follows:
按照式(Ⅰ)中各向异性磁体粉末中各元素的比例配料;According to formula (I), the proportion of each element in the anisotropic magnet powder;
将配好的原料混合在惰性气氛下进行熔炼,得到母合金;Mix the prepared raw materials in an inert atmosphere for smelting to obtain a master alloy;
将所述母合金速凝制成合金片;Rapid solidification of the master alloy into alloy flakes;
将所述合金片通过氢破、气流磨进行粉碎,得到各向异性磁体粉末。The alloy flakes are crushed by hydrogen cracking and jet mill to obtain anisotropic magnet powder.
上述熔炼、速凝、氢破和气流磨为本领域技术人员熟知的技术手段,对此本申请不进行特别的限制。The above-mentioned smelting, rapid solidification, hydrogen breaking and jet milling are technical means well known to those skilled in the art, and this application is not particularly limited.
所述重稀土粉末的制备方法具体为:The preparation method of the heavy rare earth powder is specifically as follows:
按照式(Ⅱ)中各元素的比例配料;Ingredients according to the proportion of each element in formula (II);
将配好的原料混合并在惰性气氛下进行熔炼,得到重稀土母合金;Mix the prepared raw materials and smelt in an inert atmosphere to obtain a heavy rare earth master alloy;
将所述母合金通过氢破-气流磨工艺或者球磨工艺进行粉碎,得到重稀土粉末。The master alloy is pulverized through a hydrogen breaking-jet milling process or a ball milling process to obtain heavy rare earth powder.
同样,上述熔炼、氢破和气流磨的工艺为本领域技术人员熟知的技术手段,对此本申请没有特别的限制。Likewise, the above-mentioned smelting, hydrogen breaking and jet milling processes are technical means well known to those skilled in the art, and there is no particular limitation on this application.
上述各向异性磁体粉末的粒径为1.5~3.0μm,所述重稀土粉末的粒径为 0.1~2.0μm。The anisotropic magnet powder has a particle size of 1.5 to 3.0 m, and the heavy rare earth powder has a particle size of 0.1 to 2.0 m.
在原料混合之后,则将上述得到的混合磁粉依次进行取向压型、烧结和回火,由此得到钕铁硼永磁材料;在上述过程中,所述取向压型、烧结和回火为本领域技术人员熟知的技术工艺手段,对此本申请对其工艺操作不进行特别的限制。所述取向压型具体是将所述混合磁粉在2.3~2.5T下压制成型,再于150~200MPa下静压,即得到毛坯磁体。所述烧结的温度为1060~1075℃,时间为2~4h。所述回火处理真空环境或保护气氛中依次进行的一级回火和二级回火,所述一级回火的温度为850~900℃,所述一级回火的时间为1h~3h,所述二级回火的温度为480℃~550℃,所述二级回火的时间为1h~3h。After the raw materials are mixed, the mixed magnetic powder obtained above is sequentially subjected to orientation pressing, sintering and tempering, thereby obtaining a neodymium iron boron permanent magnet material; in the above process, the orientation pressing, sintering and tempering are based Technical and technological means well known to those skilled in the art, this application does not impose special restrictions on their technological operations. The orientation molding is specifically to press and mold the mixed magnetic powder at 2.3-2.5T, and then statically press at 150-200 MPa to obtain a blank magnet. The sintering temperature is 1060-1075°C, and the time is 2-4h. The first-stage tempering and the second-stage tempering are sequentially performed in the vacuum environment or protective atmosphere of the tempering treatment, the temperature of the first-stage tempering is 850-900°C, and the time of the first-stage tempering is 1h-3h The temperature of the secondary tempering is 480°C to 550°C, and the time of the secondary tempering is 1h-3h.
本申请提供的钕铁硼永磁材料包括主相结构以及均匀分布于主相结构周围的壳层结构,所述壳层结构的成分为(Tb,Nd) 2Fe 14B,所述主相结构为(Nd,Pr) 2Fe 14B。 The neodymium iron boron permanent magnet material provided by the present application includes a main phase structure and a shell structure uniformly distributed around the main phase structure. The composition of the shell structure is (Tb, Nd) 2 Fe 14 B. The main phase structure It is (Nd, Pr) 2 Fe 14 B.
本发明提供的高性能钕铁硼永磁材料的制备方法,在剩磁不降低或者微降的情况下,可以明显地提升钕铁硼永磁材料的矫顽力同时不影响钕铁硼永磁材料的磁性能,适合大尺寸毛坯大批量生产;本发明提供的高性能钕铁硼永磁材料的制备方法,可以有效的降低重稀土的使用量。本发明提供的高性能钕铁硼永磁材料的制备方法,简单易行可以进行工业化生产。The preparation method of the high-performance neodymium iron boron permanent magnet material provided by the present invention can significantly increase the coercivity of the neodymium iron boron permanent magnet material while not affecting the neodymium iron boron permanent magnet under the condition that the remanence is not reduced or slightly reduced. The magnetic properties of the material are suitable for mass production of large-size blanks; the preparation method of the high-performance neodymium iron boron permanent magnet material provided by the present invention can effectively reduce the amount of heavy rare earth used. The preparation method of the high-performance neodymium iron boron permanent magnet material provided by the invention is simple and easy to implement and can be industrialized.
为了进一步理解本发明,下面结合实施例对本发明提供的钕铁硼磁性材料的制备方法进行详细说明,本发明的保护范围不受以下实施例的限制。In order to further understand the present invention, the preparation method of the neodymium iron boron magnetic material provided by the present invention will be described in detail below in conjunction with examples, and the protection scope of the present invention is not limited by the following examples.
实施例1Example 1
各向异性磁粉的化学式为(NdPr) 29.5Cu 0.2Al 0.1Zr 0.2Co 0.5Ga 0.1Fe bal.B 0.9,重稀土粉末的化学式为Tb 60Fe 38Al 2,重稀土粉末的掺杂量为混合磁粉的1%; The chemical formula of anisotropic magnetic powder is (NdPr) 29.5 Cu 0.2 Al 0.1 Zr 0.2 Co 0.5 Ga 0.1 Fe bal. B 0.9 , the chemical formula of heavy rare earth powder is Tb 60 Fe 38 Al 2 , and the doping amount of heavy rare earth powder is mixed magnetic powder 1%;
1)将纯度大于99%的原料按名义成分质量百分比为(NdPr) 29.5Cu 0.2Al 0.1Zr 0.2Co 0.5Ga 0.1Fe bal.B 0.9进行配比,采用速凝工艺制备出0.4毫米左右厚度的合金片,将合金片通过氢破、气流磨工艺制备出平均粒径为2μm~3μm的粉末; 1) The raw materials with a purity of more than 99% are proportioned according to the nominal component mass percentage of (NdPr) 29.5 Cu 0.2 Al 0.1 Zr 0.2 Co 0.5 Ga 0.1 Fe bal. B 0.9 , and an alloy with a thickness of about 0.4 mm is prepared by the rapid solidification process Flakes, the alloy flakes are prepared by hydrogen breaking and jet milling processes to prepare powders with an average particle size of 2 μm to 3 μm;
2)将重稀土合金按名义成分质量百分比Tb 60Fe 38Al 2进行配比经过熔炼、氢破及气流磨工艺后得到平均粒径为1μm~2μm的粉末; 2) After mixing the heavy rare earth alloy according to the nominal component mass percentage Tb 60 Fe 38 Al 2 through smelting, hydrogen breaking and jet milling processes, the powder with an average particle size of 1 μm-2 μm is obtained;
3)将重稀土粉末(Tb 60Fe 38Al 2)和各向异性磁粉按1:98的比例配比后在混 料机中混料2h~3h,将均匀混合后的粉末在2T的取向场下压制成型后,再在200MPa的液压油中进行冷等静压,得到毛坯磁体; 3) Mix the heavy rare earth powder (Tb 60 Fe 38 Al 2 ) and the anisotropic magnetic powder in a ratio of 1:98 and mix them in the mixer for 2h~3h, and place the uniformly mixed powder in the orientation field of 2T. After pressing down and forming, perform cold isostatic pressing in 200MPa hydraulic oil to obtain a blank magnet;
4)将毛坯磁体放入真空烧结炉中在1070℃烧结2h,通过气淬加风冷至室温,随后在900℃进行一级回火2h,通过气淬加风冷至室温。在500℃回火2h,完毕通过气淬加风冷,冷却至室温后出炉,即可获得钕铁硼永磁材料。4) Put the blank magnets in a vacuum sintering furnace at 1070°C for 2h, and cool to room temperature by gas quenching and air cooling, then perform one-stage tempering at 900°C for 2h, and then cool to room temperature by gas quenching and air cooling. After tempering at 500°C for 2h, after the completion of gas quenching and air cooling, after cooling to room temperature, it is out of the furnace, and the neodymium iron boron permanent magnet material can be obtained.
将制得的钕铁硼永磁材料进行测试,结果如表1所示,由表1可得,钕铁硼永磁材料的矫顽力Hcj相对于未掺杂重稀土磁粉的永磁材料高出3.18kOe,剩磁Br几乎没有变化。The prepared NdFeB permanent magnet material was tested, and the results are shown in Table 1. From Table 1, the coercivity Hcj of the NdFeB permanent magnet material is higher than that of the permanent magnet material without heavy rare earth magnetic powder. After 3.18kOe, there is almost no change in the remanence Br.
实施例2Example 2
本制备方法与实施例1的制备方法基本相同,区别在于:重稀土粉末掺杂量为混合磁粉的2%。This preparation method is basically the same as the preparation method of Example 1, except that the doping amount of the heavy rare earth powder is 2% of the mixed magnetic powder.
将制得的钕铁硼永磁材料进行测试,结果如表1所示,由表1可得,钕铁硼永磁材料的矫顽力Hcj相对于未掺杂重稀土磁粉的永磁材料高出6.54kOe,剩磁Br降低了0.19kGs。The prepared NdFeB permanent magnet material was tested, and the results are shown in Table 1. From Table 1, the coercivity Hcj of the NdFeB permanent magnet material is higher than that of the permanent magnet material without heavy rare earth magnetic powder. When the output is 6.54kOe, the remanence Br is reduced by 0.19kGs.
实施例3Example 3
本制备方法与实施例1的制备方法基本相同,区别在于:重稀土粉末掺杂量为混合磁粉的4%。This preparation method is basically the same as the preparation method of Example 1, except that the doping amount of the heavy rare earth powder is 4% of the mixed magnetic powder.
将制得的钕铁硼永磁材料进行测试,结果如表1所示,由表1可得,钕铁硼永磁材料的矫顽力Hcj相对于未掺杂重稀土磁粉的永磁材料高出10.03kOe,剩磁Br降低了1.18kGs。The prepared NdFeB permanent magnet material was tested, and the results are shown in Table 1. From Table 1, the coercivity Hcj of the NdFeB permanent magnet material is higher than that of the permanent magnet material without heavy rare earth magnetic powder. Out of 10.03kOe, the remanence Br is reduced by 1.18kGs.
表1各实施例制备的钕铁硼磁体的磁性能数据表Table 1 Data Table of Magnetic Properties of NdFeB Magnets Prepared in Each Example
Figure PCTCN2020134901-appb-000001
Figure PCTCN2020134901-appb-000001
Figure PCTCN2020134901-appb-000002
Figure PCTCN2020134901-appb-000002
对比图1和图2可以看出,图2中晶界相连续而且主相晶粒中并无明显的核壳结构,因此,掺杂了1%重稀土粉的磁体Hcj有明显提升,但是剩磁Br却没有明显变化。Comparing Figure 1 and Figure 2, it can be seen that the grain boundary phase in Figure 2 is continuous and there is no obvious core-shell structure in the main phase grains. Therefore, the Hcj of the magnet doped with 1% heavy rare earth powder has been significantly improved, but the remaining The magnetic Br did not change significantly.
对比图1、图2和图3可以看出,图3中主相晶粒存在明显的核壳结构,提高了主相晶粒的磁晶各向异性场,但重稀土元素存在于铁之间的反铁磁作用导致磁体剩磁降低。因此,掺杂了2%重稀土粉末的磁体Hcj有进一步的提升,但是剩磁略有降低。Comparing Figure 1, Figure 2 and Figure 3, it can be seen that the main phase grains in Figure 3 have an obvious core-shell structure, which improves the magnetocrystalline anisotropy field of the main phase grains, but the heavy rare earth elements exist between the iron. The anti-ferromagnetic effect of the magnet leads to a reduction in the remanence of the magnet. Therefore, the Hcj of the magnet doped with 2% heavy rare earth powder is further improved, but the remanence is slightly reduced.
对比图1、图2、图3和图4可以看出,图4中主相晶粒中核壳结构的核占比相对于图3中的要小,这表明重稀土元素更多地进入了主相晶粒,进一步提升了主相晶粒的磁晶各向异性场。因此,掺杂了4%重稀土粉末的磁体Hcj相对于掺杂了2%重稀土粉末的磁体有进一步的提升,但是剩磁降低的更明显。Comparing Figure 1, Figure 2, Figure 3 and Figure 4, it can be seen that the core-shell structure of the main phase grains in Figure 4 is smaller than that in Figure 3, which indicates that more heavy rare earth elements have entered the main phase. Phase grains further enhance the magnetocrystalline anisotropy field of the main phase grains. Therefore, the magnet Hcj doped with 4% heavy rare earth powder has a further improvement compared with the magnet doped with 2% heavy rare earth powder, but the remanence decreases more obviously.
对比例1Comparative example 1
本制备方法与实施例1的制备方法基本相同,区别在于:重稀土粉末掺杂量为混合磁粉的6%。This preparation method is basically the same as the preparation method of Example 1, except that the doping amount of the heavy rare earth powder is 6% of the mixed magnetic powder.
将制得的钕铁硼永磁材料进行测试,本对比例制备的磁体的Br为12.42KGs,Hcj为28.56KOe。由图5可知,主相晶粒中核壳结构的核进一步缩小,这表明重稀土元素掺杂过多,使得剩磁降低太厉害。The prepared neodymium iron boron permanent magnet material was tested, and the Br of the magnet prepared in this comparative example was 12.42 KGs, and the Hcj was 28.56 KOe. It can be seen from Fig. 5 that the core of the core-shell structure in the main phase grains is further reduced, which indicates that the heavy rare earth elements are doped too much, which makes the remanence decrease too much.
以上实施例的说明只是用于帮助理解本发明的方法及其核心思想。应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以对本发明进行若干改进和修饰,这些改进和修饰也落入本发明权利要求的保护范围内。The description of the above embodiments is only used to help understand the method and the core idea of the present invention. It should be pointed out that for those of ordinary skill in the art, without departing from the principle of the present invention, several improvements and modifications can be made to the present invention, and these improvements and modifications also fall within the protection scope of the claims of the present invention.
对所公开的实施例的上述说明,使本领域专业技术人员能够实现或使用本发明。对这些实施例的多种修改对本领域的专业技术人员来说将是显而易见的,本文中所定义的一般原理可以在不脱离本发明的精神或范围的情况下,在其它实施例中实现。因此,本发明将不会被限制于本文所示的这些实施例,而是要符合与本文所公开的原理和新颖特点相一致的最宽的范围。The above description of the disclosed embodiments enables those skilled in the art to implement or use the present invention. Various modifications to these embodiments will be obvious to those skilled in the art, and the general principles defined herein can be implemented in other embodiments without departing from the spirit or scope of the present invention. Therefore, the present invention will not be limited to the embodiments shown in this document, but should conform to the widest scope consistent with the principles and novel features disclosed in this document.

Claims (10)

  1. 一种钕铁硼永磁材料,由如式(Ⅰ)所示的各向异性磁体和如式(Ⅱ)所示的重稀土制备得到,所述重稀土占所述各向异性磁体和所述重稀土总量的质量比例为0.1~5wt%;A neodymium iron boron permanent magnet material, prepared from an anisotropic magnet as shown in formula (I) and a heavy rare earth as shown in formula (II), where the heavy rare earth accounts for the anisotropic magnet and the The mass ratio of the total amount of heavy rare earths is 0.1-5wt%;
    (Nd,Pr) xFe (100-x-y-z)B yM z  (Ⅰ); (Nd,Pr) x Fe (100-xyz) B y M z (Ⅰ);
    Tb aFe bAl 100-a-b  (Ⅱ); Tb a Fe b Al 100-ab (Ⅱ);
    其中,28.6wt%≤x≤29.5wt%,0.85wt%≤y≤0.9wt%,0<z≤2.5wt%,M选自Co、Al、Cu、Zr、Ti、Ni和Ga中的一种或多种;Among them, 28.6wt%≤x≤29.5wt%, 0.85wt%≤y≤0.9wt%, 0<z≤2.5wt%, M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
    60wt%≤a≤92wt%,6wt%≤b≤38wt%,a+b=100wt%。60wt%≤a≤92wt%, 6wt%≤b≤38wt%, a+b=100wt%.
  2. 根据权利要求1所述的钕铁硼永磁材料,其特征在于,所述重稀土占所述各向异性磁体和所述重稀土总量的质量比例为1wt%~2wt%。The neodymium iron boron permanent magnet material according to claim 1, wherein the mass ratio of the heavy rare earth to the total amount of the anisotropic magnet and the heavy rare earth is 1 wt% to 2 wt%.
  3. 根据权利要求1所述的钕铁硼永磁材料,其特征在于,所述M选自Co、Al、Cu、Zr和Ga。The neodymium iron boron permanent magnet material according to claim 1, wherein the M is selected from Co, Al, Cu, Zr and Ga.
  4. 根据权利要求1~3任一项所述的钕铁硼永磁材料,其特征在于,所述钕铁硼永磁材料包括主相结构和位于主相结构周围的壳层结构,所述主相结构为(Nd,Pr) 2Fe 14B,所述壳层结构为(Tb,Nd) 2Fe 14B。 The neodymium iron boron permanent magnetic material according to any one of claims 1 to 3, wherein the neodymium iron boron permanent magnetic material comprises a main phase structure and a shell structure located around the main phase structure, and the main phase The structure is (Nd, Pr) 2 Fe 14 B, and the shell structure is (Tb, Nd) 2 Fe 14 B.
  5. 权利要求1所述的钕铁硼永磁材料的制备方法,包括以下步骤:The preparation method of the neodymium iron boron permanent magnet material of claim 1, comprising the following steps:
    A)将如式(Ⅰ)所示的各向异性磁体粉末和如式(Ⅱ)所示的重稀土粉末混合,得到混合磁粉,所述混合磁粉中所述重稀土粉末的质量比例为0.1~5wt%;A) Mixing the anisotropic magnet powder as shown in formula (I) and the heavy rare earth powder as shown in formula (II) to obtain mixed magnetic powder. The mass ratio of the heavy rare earth powder in the mixed magnetic powder is 0.1~ 5wt%;
    B)将所述混合磁粉依次进行取向压型、烧结和回火,得到钕铁硼永磁材料;B) The mixed magnetic powder is oriented, pressed, sintered and tempered in sequence to obtain a neodymium iron boron permanent magnet material;
    (Nd,Pr) xFe (100-x-y-z)B yM z  (Ⅰ); (Nd,Pr) x Fe (100-xyz) B y M z (Ⅰ);
    Tb aFe bAl 100-a-b  (Ⅱ); Tb a Fe b Al 100-ab (Ⅱ);
    其中,28.6wt%≤x≤29.5wt%,0.85wt%≤y≤0.9wt%,0<z≤2.5wt%,M选自Co、Al、Cu、Zr、Ti、Ni和Ga中的一种或多种;Among them, 28.6wt%≤x≤29.5wt%, 0.85wt%≤y≤0.9wt%, 0<z≤2.5wt%, M is selected from one of Co, Al, Cu, Zr, Ti, Ni and Ga Or multiple
    60wt%≤a≤92wt%,6wt%≤b≤38wt%,a+b=100wt%。60wt%≤a≤92wt%, 6wt%≤b≤38wt%, a+b=100wt%.
  6. 根据权利要求5所述的制备方法,其特征在于,所述各向异性磁体粉 末通过氢破-气流磨工艺制备得到,所述各向异性磁体粉末的粒径为1.5~3.0μm。The preparation method according to claim 5, wherein the anisotropic magnet powder is prepared by a hydrogen breaking-jet milling process, and the particle size of the anisotropic magnet powder is 1.5-3.0 m.
  7. 根据权利要求5或6所述的制备方法,其特征在于,所述各向异性磁体粉末的制备方法具体为:The preparation method according to claim 5 or 6, wherein the preparation method of the anisotropic magnet powder is specifically:
    按照式(Ⅰ)中各向异性磁体粉末中各元素的比例配料;According to formula (I), the proportion of each element in the anisotropic magnet powder;
    将配好的原料混合在惰性气氛下进行熔炼,得到母合金;Mix the prepared raw materials in an inert atmosphere for smelting to obtain a master alloy;
    将所述母合金速凝制成合金片;Rapid solidification of the master alloy into alloy flakes;
    将所述合金片通过氢破、气流磨进行粉碎,得到各向异性磁体粉末。The alloy flakes are crushed by hydrogen cracking and jet mill to obtain anisotropic magnet powder.
  8. 根据权利要求5所述的制备方法,其特征在于,所述重稀土粉末的制备方法具体为:The preparation method according to claim 5, wherein the preparation method of the heavy rare earth powder is specifically:
    按照式(Ⅱ)中各元素的比例配料;Ingredients according to the proportion of each element in formula (II);
    将配好的原料混合并在惰性气氛下进行熔炼,得到重稀土母合金;Mix the prepared raw materials and smelt in an inert atmosphere to obtain a heavy rare earth master alloy;
    将所述母合金通过氢破-气流磨工艺或者球磨工艺进行粉碎,得到重稀土粉末;所述的重稀土粉末的粒径为0.1μm~2μm。The master alloy is pulverized through a hydrogen breaking-jet milling process or a ball milling process to obtain heavy rare earth powder; the particle size of the heavy rare earth powder is 0.1 μm-2 μm.
  9. 根据权利要求5所述的制备方法,其特征在于,所述取向压型具体为:The preparation method according to claim 5, characterized in that the orientation pressing is specifically:
    将所述混合磁粉在2.3~2.5T压制成型,再于150~200MPa静压,得到毛坯磁体。The mixed magnetic powder is press-formed at 2.3-2.5T, and then statically pressed at 150-200 MPa to obtain a blank magnet.
  10. 根据权利要求5所述的制备方法,其特征在于,所述烧结的温度为1060℃~1075℃,所述烧结的时间为2~4h,所述回火处理包括真空环境或保护气氛中依次进行的一级回火和二级回火,所述一级回火的温度为850~900℃,所述一级回火的时间为1h~3h,所述二级回火的温度为480℃~550℃,所述二级回火的时间为1h~3h。The preparation method according to claim 5, wherein the sintering temperature is 1060° C. to 1075° C., the sintering time is 2 to 4 hours, and the tempering treatment includes successively performing in a vacuum environment or a protective atmosphere. The first-stage tempering and the second-stage tempering, the temperature of the first-stage tempering is 850~900℃, the time of the first-stage tempering is 1h~3h, and the temperature of the second-stage tempering is 480℃~ At 550°C, the time for the secondary tempering is 1h-3h.
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