Low-cost Sm0.7Y0.3Co5 sintered magnet produced by traditional powder metallurgical techniques
College of Materials Science and Engineering,Key Laboratory of Advanced Functional Materials,Ministry of Education of China,Beijing University of Technology
作者简介:*Ming Yue e-mail:yueming@bjut.edu.cn;
收稿日期:16 October 2018
基金:financially supported by the State Key Program of Natural Science Foundation of China (Nos. 51331003 and 51871005);the International S&T Cooperation Program of China (No.2015DFG52020);
Low-cost Sm0.7Y0.3Co5 sintered magnet produced by traditional powder metallurgical techniques
Dong-Tao Zhang Nai-Xing Cai Rong-Chun Zhu Wei-Qiang Liu Ming Yue
College of Materials Science and Engineering,Key Laboratory of Advanced Functional Materials,Ministry of Education of China,Beijing University of Technology
Abstract:
RCo5(R=rare earth) sintered magnets have good temperature stability,so it is still widely used in high temperature field.In this paper,by the method of adding liquid phase SmCo1.7 to the main phase,Sm0.7Y0.3Co5 magnet was prepared by traditional powder metallurgical process.The results show the presence of a main phase RCo5,a minor phase R2 Co7,and a R-rich phase in the magnet.Contrasting the results of the XRD(X-ray diffraction) in random and oriented directions,the magnet has a well-aligned(00l) orientated texture,which is consistent with the result of the electron backscattered diffraction(EBSD).The Sm0.7Y0.3Co5 sintered magnet has good magnetic properties as remanence(Br) is 0.96 T,the coercivity(Hcj) is 1201.96 kA·m-1,and maximum magnetic energy product((BH)max) is 175.16 kJ m-3.
Keyword:
Sm0.7Y0.3Co5; Sintered magnets; Low-cost; Magnetic properties; RCo5;
Received: 16 October 2018
1 Introduction
RCo5 (R=rare earth) alloys have favorable intrinsic magnetic properties for high temperature application
Therefore,the major motivation for this work is to obtain high performance Sm1-xYxCo5 magnet with lower cost and further understand the relationship between magnetic properties and microstructure of Sm1-xYxCo5magnet after doping Y.As the density and HA of the YCo5compound are low,so the replacement amount of Sm by Y atoms can not be high.In this paper,Sm0.7Y0.3Co5 magnet was prepared by traditional powder metallurgical techniques.Moreover,SmCo1.7 alloy as a liquid phase was also added into the Sm0.7Y0.3Co5 magnet,which can improve the density of the magnet and decrease the sintering temperature during processing.
2 Experimental
The Sm0.7Y0.3Co4.8 and SmCo1.7 ingots were prepared by induction melting in high-purity argon atmosphere.Excess Sm of 5 wt%and Y of 5 wt%were added to compensate for weight loss due to evaporation.The two ingots were crushed into powders with a size of 3-5μm by a jaw crusher,a disk mill and a rolling ball mill,respectively.The weight ratio of the balls to the powders was 5:1,the milling time was 7 h,and the ball-mill medium was gasoline.The Sm0.7Y0.3Co4.8 powders,mixed with the SmCo1.7 powders of 6 wt%,were orientated in a magnetic field of 2 T,then isostatic ally cold-pressed under a pressure of 220 MPa.Finally,the sample was sintered at 1150℃in argon for 1 h,cooled down to 850℃at a rate of1℃·min-1 and held for 1.5 h,then fast cooled in air to room temperature.This process is schematically shown in Fig.1.
The crystal structure of the sample was analyzed by X-ray diffraction (XRD,Rigaku Dmax-C) using Cu Kαradiation.The sample with a size of 7 mm×7 mm×15 mm was magnetized in a 10-T magnetic field along the easy magnetization axis,and measured by the NIM-500C BH looper.The elemental distribution of the sample was identified by the electron probe micro-analyzer (EPMA,EPMA-1720H).The microstructure of the sample was analyzed by scanning electron microscopy (SEM,FEI NANO200) with energy-dispersive spectrometer (EDS)and transmission electron microscope (TEM,JEOL-200C).The density of the sample was measured by the Archimedes method.The electron backscattered diffraction(EBSD) data was collected by EBSD detector (Hikari ED AX) incorporated in SEM (FEI Quanta 250,USA),and the measurement surface of the samples is perpendicular to the easy axis of the magnet.The EBSD data were analyzed by the TSL OIM Analysis 5.3 software (EDAX Inc,USA).The multiple of random distribution (MRD) of inverse pole figure (IPF) maps and pole figures (PF) revealed the orientation of the sample.Magnetic domains of the sample during the magnetization and demagnetization processes were observed by a magneto-optical Kerr optical microscope (MOKE,BH-786IP-PK).
Fig.1 Sintering process curve of Sm0.7Y0.3Co5 magnet
3 Results and discussion
Figure 2 shows the random and oriented XRD patterns of the Sm0.7Y0.3Co5 magnets,the data of the random magnet are from the crushed powders and the data of the oriented magnet are from the aligned magnet of the Sm0.7Y0.3Co5sintered magnet.For the random magnet,main phase of RCo5,minor phase of R2Co7 and a trace of R-rich phase exist in the magnet.After orientation,the (00l) peaks become very strong,while the (101) and (111) peaks become weak and other peaks almost disappear in the oriented magnet.The intensity ratio of (002) to (111)peaks,I(002)/I(111),can be used to characterize texture degree in the Sm0.7Y0.3Co5 magnet.The value ofI(002)/I(111) changes from 0.2 to 60.2 before and after orientation,indicating an excellent orientation texture in the magnet.
Figure 3 shows the demagnetization curves of the magnet in a temperature range of 25-200℃,and the magnetic properties are listed in Table 1.It can be seen that the demagnetization curve still maintains an acceptable square shape at 25℃for the Y-containing magnet.The maximum magnetic energy product((BH)max),remanence (Br) and coercivity (Hcj) of the magnet are175.16 kJ·m-3,0.96 T and 1201.96 kA·m-1 at 25℃.The density of the sintered magnet is 8.0 g·cm-3,but the theoretical density of the Sm0.7Y0.3Co5 magnet is 8.2 g·cm-3,so the density,remanence and magnetic energy product of the magnet still have potential to be improved.As the temperature increases,the (BH)max,Br and Hcj of the magnet decreases to 113.9 kJ·m-3,0.86 T and437.8 kA·m-1 at 200℃.Therefore,the remanence temperature coefficient (a) and the coercivity temperature coefficient (β) are-0.06%.℃-1 and-0.37%·℃-1 in a temperature range of 25-200℃,respectively.However,along with the rise in temperature,the B-H curves are not straight,because there are 2:7 phases in the magnet and they are easier to demagnetize and nucleate than 1:5 phase at high temperature,indicating that the magnetic properties of the magnet need to be improved.
Fig.2 XRD patterns of random and oriented Sm0.7Y0.3Co5 magnets
Fig.3 Demagnetization curves of Sm0.7Y0.3 Co5 magnet in a tem-perature range of 25-200℃
Table 1 Magnetic properties of Sm0.7Y0.3Co5 magnet in a tempera-ture range of 25-200℃
Figure 4 shows morphology images of the Sm0.7Y0.3Co5magnet.It can be seen in Fig.4a that the magnet is mainly composed of three phases.It can be seen from Fig.4b that the dark gray areas (Area 1) are the main phase,the light gray areas (Area 2) are the secondary phase,and the dark areas (Area 3) are the R-rich phase which are easy to fall out,and that the distributions of each phase in the magnet are uniform.EDS results at different areas in Fig.4b are shown in Table 2.It can be concluded from Fig.4b that the large dark gray areas marked as 1 are the main RCo5 phase,the light gray areas marked as 2 are the minor R2Co7 phase,and the black hole areas marked as 3 are the R-rich phase,in agreement with XRD results.It is not good that there are excessive R2Co7 phases in the magnet.According to the phase diagram,an excess of Sm is required to avoid the formation of the Sm2Co17 phase
The results of XRD and EPMA show that there are three phases:the 1:5 main phase,the 2:7 minor phase and the R-rich phase in the magnet.The partial replacement of Y by Sm atoms does not change the structure.Therefore,EBSD analysis was conducted by setting SmCo5 and Sm2Co7 as the identification phases,as shown in Fig.6.The orientation of the grains is based on the orientation of the hexagonal symmetry of the RCo5 phase.The oriented grain images can distinguish grains with different orientations.Compared with a standard map,it can be seen that the diffraction patterns of both 1:5 phase (Area 1) and 2:7phase (Area 2) are similar to red,indicating that the grain orientation is very close to (00l),which is in accordance with the results of XRD.The high orientation degree is very helpful in improving the remanence of the magnets
Fig.4 BSE images of Sm0.7Y0.3Co5 magnet with different magnifications
Table 2 Elemental content at different areas of Sm0.7Y0.3Co5 magnet(at%)
Fig.5 EPMA results of Sm0.7Y0.3Co5 magnet:a SEM image,b Sm,c Y,and d Co
Fig.6 IPF maps of Sm0.7Y0.3Co5 magnet:a BSE of a selected region and b 1:5 and 2:7 with orientation legend for hexagonal symmetries
Fig.7 (0001) pole figure and inverse pole figures of normal direction (ND) of a,c 1:5 phase and b,d 2:7 phase
Figure 8 shows the magnetic domain and backscattered electron morphology (BSEM) in situ observations by MOKE and SEM,respectively.The direction of themagnetic field is consistent with c-axis.In Fig.8a,the dark gray phase (Area 1) and light gray phase (Area 2) are the1:5 and 2:7 phases,respectively.Figure 8b indicates the magnetic domains of the magnet at thermal demagnetization state.The domains in the dark gray areas are pided into two directions.The dark part is in one direction,the light part is in the reverse direction,and the magnetic domain is a maze-like domain (Area 1);the width of the domain is about 5μm.However,in the light gray 2:7 phase areas,for example,Area 2,there is no obvious domain.The magnetic domain,at remanent magnetization state after magnetization by a 10-T magnetic field,is shown in Fig.8c.All the domains in the 1:5 phase areas move to the same direction,and there are no domains in the field of vision.In Fig.8d,partial magnetic domain reversal occurs in the 1:5 phase areas when a-875.6 kA·m-1 reverse field is applied.For the 2:7 phase areas,in the thermal demagnetization state,remanent magnetization state or applying a reversal magnetic field,there is no change of magnetic domain.The reason needs to be further clarified.The magnetic domain evolution during demagnetization process is shown in Fig.9,and the magnetic reversal field is 0,-398,-716.4,and-1114.4 kA·m-1.The direction of the magnetic field is consistent with c-axis.When the magnetization field is 0 kA·m-1 (remanence),the magnetic domain is a single domain state.When the reverse magnetization field is-398 kA·m-1,a small number of reverse domains start to appear.With further increase in the reverse field (-716.4 and-1114.4 kA·m-1),new reverse domains appear and their number increases.Moreover,the appearance of the reverse domains is irreversible.
Fig.8 a Magnetic domain SEM image of Sm0.7Y0.3Co5 magnet in situ;MOKE images b at thermal demagnetization state,c at remanent magnetization state after magnetization by a magnetic field of 10 T and d under a 875.6 kA·m-1 reverse magnetic field (analyzed surface perpendicular to orientation direction of magnet)
Fig.9 MOKE images of Sm0,7Y0,3Co5 magnet at applied filed of a 0 kA·m-1,b-398 kA·m-1,c-716.4 kA·m-1 and d-1114.4 kA·m-1during demagnetization process
Fig.10 a TEM image of Sm0.7Y0.3Co5 magnet,b typical high-resolution TEM image of Area 1 and c typical high-resolution TEM image ofArea 2
TEM analysis of the Sm0.7Y0.3Co5 magnet is shown in Fig.10.Figure 10a is a typical bright-field TEM morphology.There is no complete grain in the TEM vision because the grain size is about 8μm.Figure 10b shows the high-resolution image of Area 1,which is identified as SmCo5 phase with hexagonal structure.The high-resolution image of Area 2 in Fig.10c indicates that it is Sm2O3with the monoclinic structure.The grain size of the Sm2O3is about 100 nm.
4 Conclusion
The Sm0.7Y0.3Co5 magnet was successfully prepared by traditional powder metallurgical process.The Sm0.7Y0.3Co5 magnet bears optimal magnetic properties with Br=0.96 T,Hcj=1201.96 kA·m-1 and(BH)max=175.16 kJ·m-3.There are three coexisting phases composed of 1:5 main phase,2:7 minor phase and a R-rich phase in the magnet.The magnet has a well-aligned(00l) orientation texture.The magnetic domain of the 1:5phase is a maze domain.There is no obvious magnetic domain in the 2:7 phase.
参考文献
[26] Strnat KJ,Strnat RMW.Rare earth-cobalt permanent magnets.J Magn Magn Mater.1991;100(1):38.