Patent Application
20220319773
The present disclosure relates to the field of permanent magnets, and in particular to a grain boundary diffusion method for a bulk rare earth permanent magnetic material.
Neodymium iron boron (NdFeB) has excellent comprehensive magnetic properties and is widely used in fields such as energy, information, transportation, and national defense. NdFeB is one of the most important rare earth functional materials and one of the key basic materials for the national economy. However, sintered NdFeB shows poor temperature stability and has a working temperature usually lower than 100° C., which greatly limits its applications in electric vehicles, wind power, and aerospace. At present, the use of cheap and high-abundance rare earths La/Ce/Y to replace the expensive Nd/Pr/Dy/Tb greatly reduces the raw material cost of rare earth permanent magnets, which has gained widespread attention inside and outside China. However, the intrinsic magnetism of a 2:14:1 phase formed by lanthanum, cerium, and yttrium is weaker than that of Nd2Fe14B, and the magnetic dilution of a high-abundance rare earth permanent magnet is significant. Specifically, the coercivity is low, which cannot meet the commercial requirements. This problem is difficult to solve, which has restricted the development and application of high-abundance rare earth permanent magnets for a long time.
At present, methods for improving the coercivity of NdFeB mainly include: 1) Addition of heavy rare earths through smelting. However, the introduction of a large amount of uniformly-distributed Dy/Tb into a main phase not only greatly increases the raw material cost due to the consumption of scarce heavy rare earth resources, but also greatly reduces the remanence and magnetic energy product. 2) Grain refinement. However, the magnetic powders are easily oxidized after a grain size to 3 μm or smaller, which decrease the coercivity unfortunately. 3) Grain boundary diffusion. This method can greatly improve the coercivity of NdFeB magnets, involves simple operations, and can realize the efficient utilization of rare earths. Therefore, grain boundary diffusion is currently a research hotspot. However, due to the limited element diffusion depth, the conventional grain boundary diffusion method is merely suitable for magnets with a thickness of less than 5 mm, and thus the large-scale application is limited. How to improve a grain boundary diffusion depth and develop a grain boundary diffusion method for a bulk rare earth permanent magnetic material is currently a research challenge in the field of rare earth permanent magnets.
In order to overcome the deficiencies of the prior art, the present disclosure provides a grain boundary diffusion method for a bulk rare earth permanent magnetic material, including the following steps:
(1) fabricating an initial magnet by a sintering, hot pressing, or hot deformation process;
(2) loading a grain boundary diffusion alloy source on a surface of the initial magnet; (3) placing the initial magnet loaded with the alloy source in a spark plasma sintering (SPS) device, and heating the initial magnet loaded with the alloy source at a heating rate of 20° C./min to 400° C./min in the SPS device to allow grain boundary diffusion for 20 min to 180 min at a diffusion temperature of 400° C. to 900° C., a pressure of 2 MPa to 50 MPa, and a vacuum degree of less than 10−3 Pa to obtain a final magnet.
The final magnet fabricated in step (3) may have a composition of (RxA1-x)yQbalMzBw, where R is one or more selected from the group consisting of high-abundance rare earth elements La, Ce, and Y; A is one or more selected from the group consisting of lanthanide rare earth elements other than La, Ce, and Y; Q is one or more selected from the group consisting of Fe, Co, and Ni; M is one or more selected from the group consisting of Al, Cr, Cu, Zn, Ga, Ge, Mn, Mo, Nb, P, Pb, Si, Ta, Ti, V, Zr, O, F, N, C, S, and H; B is boron; and x, y, z, and w satisfy the following relationships: 0≤x≤0.8, 26≤y≤36, 1≤z≤10, and 0.8≤w≤1.3.
The initial magnet fabricated in step (1) may have a composition of (R′aA′1-a)bQ′balM′cBd, where R′ is one or more selected from the group consisting of high-abundance rare earth elements La, Ce, and Y; A′ is one or more selected from the group consisting of lanthanide rare earth elements other than La, Ce, and Y; Q′ is one or more selected from the group consisting of Fe, Co, and Ni; M′ is one or more selected from the group consisting of Al, Cr, Cu, Zn, Ga, Ge, Mn, Mo, Nb, P, Pb, Si, Ta, Ti, V, Zr, O, F, N, C, S, and H; B is boron; and a, b, c, and d satisfy the following relationships: 0≤a≤0.8, 23≤b≤33, 0.5≤c≤8, and 0.9≤d≤1.4.
The grain boundary diffusion alloy source in step (2) may have a composition of R″uM″1-u, where R″ is one or more selected from the group consisting of lanthanide rare earth elements; M″ is one or more selected from the group consisting of Fe, Co, Ni, Al, Cr, Cu, Zn, Ga, Ge, Mn, Mo, Si, Ti, O, F, and H; and u satisfies the following relationship: 0≤u≤1.
In step 2, a method for loading the grain boundary diffusion alloy source may include: electrodeposition, chemical vapor deposition (CVD), physical vapor deposition (PVD), direct physical contact, or adhesive bonding.
Compared with the prior art, the present disclosure has the following beneficial effects:
1) The present disclosure conducts grain boundary diffusion based on SPS. During a heating process, due to the influence of current, plasma, and pressure, an elemental diffusion coefficient can be increased, and a high-speed channel for diffusion appears in the magnet, which accelerates the infiltration of rare earth and alloy elements into the magnet (at a grain boundary or inside a grain), thereby enhancing a diffusion depth of elements and significantly improving the magnetic properties. It also fully utilizes the characteristic interdiffusion behaviors of abundant rare earth elements La, Ce, Y that are different from other rare earth elements to enhance the magnetic properties. Thus, a grain boundary diffusion method for a bulk rare earth permanent magnetic material is obtained, with a substitution amount of La, Ce, and Y as high as 80%.
2) The present disclosure utilizes the characteristics of SPS such as high heating rate and short heating time to suppress the grain growth during a diffusion process and thus improve the coercivity of a magnet.
The present disclosure will be further described below in conjunction with specific examples, but the present disclosure is not limited to the following examples.
An initial magnet (Pr0.12Nd0.48Ce0.4)30.8FebalCu0.3Al0.2Ga0.2Zr0.3B1.05 with a height of 25 mm was fabricated by a sintering process; a grain boundary diffusion alloy powder Nd80Al20 was loaded on a surface of the initial magnet through direct contact; and the initial magnet was placed in a SPS device and then heated at a heating rate of 400° C./min to allow grain boundary diffusion for 40 min at a diffusion temperature of 700° C. and a pressure of 20 MPa to obtain a final magnet with the following magnetic properties: Br=12.4 kG, hcj=15.5 kOe, and (BH)max=36.6 MGOe.
An initial magnet (Nd0.4La0.2Ce0.4)32FebalNb0.3Ti0.2Ga0.5Co0.3B0.9 with a height of 20 mm was fabricated by a sintering process; a grain boundary diffusion alloy powder NdH3 was loaded on a surface of the initial magnet through polyvinylpyrrolidone (PVP) adhesive bonding; and the initial magnet was placed in an SPS device and then heated at a heating rate of 20° C./min to allow grain boundary diffusion for 100 min at a diffusion temperature of 900° C. and a pressure of 50 MPa to obtain a final magnet with the following magnetic properties: Br=12.2 kG, hcj=12.5 kOe, and (BH)max=33.4 MGOe.
An initial magnet (Nd0.5Y0.1Ce0.4)30FebalZr0.15Cu0.3Co0.5Al0.2B1.01 with a height of 10 mm was fabricated by a hot deformation process; a grain boundary diffusion alloy powder Nd70Cu30 was loaded on a surface of the initial magnet through PVP adhesive bonding; and the initial magnet was placed in an SPS device and then heated at a heating rate of 400° C./min to allow grain boundary diffusion for 60 min at a diffusion temperature of 600° C. and a pressure of 2 MPa to obtain a final magnet with the following magnetic properties: Br=11.3 kG, Hcj=16.5 kOe, and (BH)max=28.2 MGOe.
An initial magnet (Pr0.18Nd0.72Ce0.1)36FebalMo0.15Al0.15Cu0.2Zr0.2B0.95 with a height of 18 mm was fabricated by a sintering process; a grain boundary diffusion alloy source Dy20Pr60Al20 was loaded on a surface of the initial magnet through magnetron sputtering; and the initial magnet was placed in an SPS device and then heated at a heating rate of 400° C./min to allow grain boundary diffusion for 180 min at a diffusion temperature of 800° C. and a pressure of 25 MPa to obtain a final magnet with the following magnetic properties: Br=12.5 kG, Hcj=25.4 kOe, and (BH)max=39.2 MGOe.
An initial magnet (Nd0.2Ce0.8)26FebalZr0.1Cu0.2Co0.5Al0.3Si0.1B1.0 with a height of 8 mm was fabricated by a hot deformation process; a grain boundary diffusion alloy powder Pr70Cu30 was loaded on a surface of the initial magnet through magnetron sputtering; and the initial magnet was placed in an SPS device and then heated at a heating rate of 100° C./min to allow grain boundary diffusion for 20 min at a diffusion temperature of 650° C. and a pressure of 5 MPa to obtain a final magnet with the following magnetic properties: Br=10.1 kG, Hcj=11.2 kOe, and (BH)max=20.3 MGOe.
An initial magnet (Pr0.14Nd0.56La0.1Ce0.2)36FebalGa0.35Al0.25Cu0.2Zr0.15B0.93 with a height of 60 mm was fabricated by a sintering process; a grain boundary diffusion alloy source Pr80Al20 was loaded on a surface of the initial magnet through magnetron sputtering; and the initial magnet was placed in an SPS device and then heated at a heating rate of 400° C./min to allow grain boundary diffusion for 180 min at a diffusion temperature of 700° C. and a pressure of 25 MPa to obtain a final magnet with the following magnetic properties: Br=12.6 kG, Hcj=18.2 kOe, and (BH)max=38.2 MGOe.
| Number | Date | Country | Kind |
|---|---|---|---|
| 201911423881.7 | Dec 2019 | CN | national |
This application is a continuation-in-part application of International Application No. PCT/CN2020/141348, filed on Dec. 30, 2020, which is based upon and claims priority to Chinese Patent Application No. 201911423881.7, filed on Dec. 31, 2019, the entire contents of which are incorporated herein by reference.
| Number | Date | Country | |
|---|---|---|---|
| Parent | PCT/CN2020/141348 | Dec 2020 | US |
| Child | 17842923 | US |
