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1.
Fe-Dy非晶膜晶化过程中结构及磁性变化SCIEI   总被引:2,自引:0,他引:2  
王佩璇  李胜利 《金属学报》1994,30(3):B116-B120
用真空双源蒸镀法在NaCl和Si单晶衬底上制备Fe,Dy成分调制多层膜.研究了非晶膜晶化过程,等温退火后多层膜结构及磁性变化。结果表明,在200℃以下退火,其沉积态非晶和成分调制结构几乎不变;300℃开始晶化,首先出现Fe晶核,随温度升高,Fe,Dy逐步晶化,600℃全部形成晶态bcc-Fe和hcp-Dy.饱和磁化强度Ms对非晶Fe,Dy膜晶化时Fe晶核的形成十分散感,而只有Fe晶粒的长大才导致矫顽力Hc增加.  相似文献   

2.
电子束加热时Fe—Dy多层膜的稳定性   总被引:2,自引:0,他引:2  
用真空双源蒸镀法在NaCl单晶衬底上制备了金属Fe-Dy(镝)多层膜,用透射电镜(TEM)分析结构。结果表明,当Fe单层厚度≥2.4nm时,Fe为bcc结构,无明显择尤取向特征;Dy单层厚度<2.4nm时,Dy为非晶态,在透射电镜样品台上经100KV加速的高强度电子束流加热多层膜,非晶Dy首先晶化变为hcp结构,随加热时间的延长,晶粒长大。150S时Fe晶粒尺寸约300nm,此时出现了铁镝氧化物。  相似文献   

3.
用真空双源蒸镀法在NaC1单晶衬底上制备了金属Fe-Dy(镝)多层膜,用透射电镜(TEM)分析结构。结果表明,当Fe单层厚度≥2.4nm时,Fe为bcc结构,无明显择尤取向特征;Dy单层厚度<2.4nm时,Dy为非晶态。在透射电镜样品台上经100kv加速的高强度电子束流加热多层膜,非晶Dy首先晶化变为hcp结构,随加热时间的延长,晶粒长大。150s时Fe晶粒尺寸约300nrn,此时出现了铁镝氧化物。  相似文献   

4.
由Miedema半经验公式计算的Fe/Y二元系自由能图,及退火时Fe/Y非晶多层膜晶化过程的XRD分析结果得出:Fe、Y晶态自由能低于初始非晶态为晶化提供驱动力,形核势垒及临界晶核尺寸控制晶化反应的相选择。  相似文献   

5.
用真空双源蒸镀法在Si单晶衬底上制备了Fe,Dy原子数比为3:2的Fe─Dy成分调制多层膜.用AES、RBS、X射线衍射(XRD)以及磁性测量分析了Ar~(+)混合前后Fe─Dy多层膜的相交.Ar~(+)离子注入能量110keV,剂量5×10~(15)─1×10~(17)/cm~2.结果表明,注入剂量为1×10~(17)/cm~2时,Fe,Dy完全混合,并且由晶态的Fe,Dy完全转变为Fe_(60)Dy_(40)(近似于该化学配比)的非晶态合金,随Ar~(+)注入量的增加,Fe一Dy多层膜的M_s下降,在剂量50×10~(15)/cm~2时下降幅度最大。  相似文献   

6.
用真空双源蒸镀法在Si单晶衬底上制备了Fe,Dy原子数比为3:2的Fe─Dy成分调制多层膜.用AES、RBS、X射线衍射(XRD)以及磁性测量分析了Ar~(+)混合前后Fe─Dy多层膜的相交.Ar~(+)离子注入能量110keV,剂量5×10~(15)─1×10~(17)/cm~2.结果表明,注入剂量为1×10~(17)/cm~2时,Fe,Dy完全混合,并且由晶态的Fe,Dy完全转变为Fe_(60)Dy_(40)(近似于该化学配比)的非晶态合金,随Ar~(+)注入量的增加,Fe一Dy多层膜的M_s下降,在剂量50×10~(15)/cm~2时下降幅度最大。  相似文献   

7.
李胜利  阎凤章 《金属学报》1994,30(4):A160-A163
用真空双源蒸镀法在Si单晶衬底上制备了Fe,Dy原子数比为3:2的Fe─Dy成分调制多层膜.用AES、RBS、X射线衍射(XRD)以及磁性测量分析了Ar^(+)混合前后Fe─Dy多层膜的相交.Ar^(+)离子注入能量110keV,剂量5×10^(15)─1×10^(17)/cm~2.结果表明,注入剂量为1×10^(17)/cm~2时,Fe,Dy完全混合,并且由晶态的Fe,Dy完全转变为Fe_(60)Dy_(40)(近似于该化学配比)的非晶态合金,随Ar^(+)注入量的增加,Fe一Dy多层膜的M_s下降,在剂量50×10^(15)/cm~2时下降幅度最大。  相似文献   

8.
研究了添加Dy和Nb对纳米复合Pr2Fe14B/α-Fe永磁合金形成、组织结构及磁性能的影响。研究表明,对于三元的Pr9Fe85B6非晶带的晶化过程,在α-Fe相初始晶化之后,晶化最终产物Pr2Fe14B+α-Fe形成之前出现Pr2Fe23B3亚稳相。而添加Dy或同时添加Dy和Nb后晶化过程不出现亚稳相。添加Dy和Nb元素显著地提高了纳米复合永磁合金的磁性能。  相似文献   

9.
通过比较Fe/RE非晶多层膜中所有成分范围内非晶合金形成焓△H^am与固溶体形成焓△H^SS得出,在△H^am〈△H^SS成分范围内的非晶与在△H^am〉△H^SS成分范围内非晶的晶化方式及晶化温度不同。这从理论上系统地解释了多层膜晶化为一个缓慢过程,没有确定的晶化温度。  相似文献   

10.
对Fe78Si13B9、Fe77Cu1Si13B9和Fe74Cu1Nb3Su13B9三种非晶合金的晶化过程进行了DTA热分析和在位动态电镜观察.在Fe77Cu13B9非晶的晶化前期阶段,发现了条状调幅结构,这被认为是Cu元素Fe基非晶基体中的Spinodal分解的产物,富Cu区还可以作为α-Fe晶核的产床,导致了高密度形核.  相似文献   

11.
In as-welded state, each region of 2219 aluminum alloy TIG-welded joint shows diff erent microstructure and microhardness due to the diff erent welding heat cycles and the resulting evolution of second phases. After the post-weld heat treatment, both the amount and the size of the eutectic structure or θ phases decreased. Correspondingly, both the Cu content in α-Al matrix and the microhardness increased to a similar level in each region of the joint, and the tensile strength of the entire joint was greatly improved. Post-weld heat treatment played the role of solid solution strengthening and aging strengthening. After the post-weld heat treatment, the weld performance became similar to other regions, but weld reinforcements lost their reinforcing eff ect on the weld and their existence was more of an adverse eff ect. The joint without weld reinforcements after the post-weld heat treatment had the optimal tensile properties, and the specimens randomly crack in the weld zone.  相似文献   

12.
After nearly two years' tense construction, the first phase of industrialized base of Shenyang Research Institute of Foundry (SRIF), located at the Tiexi Casting and Forging Industrial Park in the west of Tiexi District, has now been completed and formally put into operation.  相似文献   

13.
Institute of Process Engineering, Chinese Academy of Sciences, China, has proposed a method for oxidative leaching of chromite with potassium hydroxide. Understanding the mechanism of chromite decomposition, especially in the potassium hydroxide fusion, is important for the optimization of the operating parameters of the oxidative leaching process. A traditional thermodynamic method is proposed and the thermal decomposition and the reaction decomposition during the oxidative leaching of chromite with KOH and oxygen is discussed, which suggests that chromite is mainly destroyed by reactions with KOH and oxygen. Meanwhile, equilibrium of the main reactions of the above process was calculated at different temperatures and oxygen partial pressures. The stable zones of productions, namely, K2CrO4 and Fe2O3, increase with the decrease of temperature, which indicates that higher temperature is not beneficial to thermodynamic reactions. In addition, a comparison of the general alkali methods is carried out, and it is concluded that the KOH leaching process is thermodynamically superior to the conventional chromate production process.  相似文献   

14.
The effect of isochronal heat treatments for 1h on variation of damping, hardness and microstructural change of the magnesium wrought alloy AZ61 was investigated. Damping and hardness behaviour could be attributed to the evolution of precipitation process. The influence of precipitation on damping behaviour was explained in the framework of the dislocation string model of Granato and Lücke.  相似文献   

15.
The Lanthanum-doped bismuth ferrite–lead titanate compositions of 0.5(Bi LaxFe1-xO3)–0.5(Pb Ti O3)(x = 0.05,0.10,0.15,0.20)(BLxF1-x-PT) were prepared by mixed oxide method.Structural characterization was performed by X-ray diffraction and shows a tetragonal structure at room temperature.The lattice parameter c/a ratio decreases with increasing of La(x = 0.05–0.20) concentration of the composites.The effect of charge carrier/ion hopping mechanism,conductivity,relaxation process and impedance parameters was studied using an impedance analyzer in a wide frequency range(102–106Hz) at different temperatures.The nature of Nyquist plot confirms the presence of bulk effects only,and non-Debye type of relaxation processes occurs in the composites.The electrical modulus exhibits an important role of the hopping mechanism in the electrical transport process of the materials.The ac conductivity and dc conductivity of the materials were studied,and the activation energy found to be 0.81,0.77,0.76 and 0.74 e V for all compositions of x = 0.05–0.20 at different temperatures(200–300 °C).  相似文献   

16.
The orientation relationships(ORs)between the martensite and the retained austenite in low-and medium-carbon steels after quenching–partitioning–tempering process were studied in this work.The ORs in the studied steels are identified by selected-area electron diffraction(SAED)as either K–S or N–W ORs.Meanwhile,the ORs were also studied based on numerical fitting of electron backscatter diffraction data method suggested by Miyamoto.The simulated K–S and N–W ORs in the low-index directions generally do not well coincide with the experimental pole figure,which may be attributed to both the orientation spread from the ideal variant orientations and high symmetry of the low-index directions.However,the simulated results coincide well with experimental pole figures in the high-index directions{123}_(bcc).A modified method with simplicity based on Miyamoto’s work was proposed.The results indicate that the ORs determined by modified method are similar to those determined by Miyamoto’method,that is,the OR is near K–S OR for the low-carbon Q–P–T steel,and with the increase of carbon content,the OR is closer to N–W OR in medium-carbon Q–P–T steel.  相似文献   

17.
On the basis of the single-particle framework, a new theory on inclusion growth in metallurgical melts is developed to study the kinetics of inclusion growth on account of reaction and collision. The studies show that the early growth of inclusion depends on reaction growth and Brawnian motion collision, and where the former is decisive, the late growth depends on turbulence collision and Stokes' collision, and where the former is dominant; collision growth is very quick during the smelting process, lessened in the refining process, but nearly negligible in the continuous casting process.  相似文献   

18.
The motion of melt droplets in spray degassing process was analyzed theoretically. The height of the treatment tank in spray degassing process could be determined by the results of theoretical calculation of motion of melt droplets. To know whether the melt droplets would solidify during spraying process, the balance temperature of melt droplets was also theoretically analyzed. Then proof experiments for theoretical results about temperature of melt droplets were carried. In comparison, the experimental results were nearly similar to the calculation results.  相似文献   

19.
This work was to reveal the residual stress profile in electron beam welded Ti-6Al-4V alloy plates(50 mm thick) by using finite element and contour measurement methods.A three-dimensional finite element model of 50-mmthick titanium component was proposed,in which a column–cone combined heat source model was used to simulate the temperature field and a thermo-elastic–plastic model to analyze residual stress in a weld joint based on ABAQUS software.Considering the uncertainty of welding simulation,the computation was calibrated by experimental data of contour measurement method.Both test and simulated results show that residual stresses on the surface and inside the weld zone are significantly different and present a narrow and large gradient feature in the weld joint.The peak tensile stress exceeds the yield strength of base materials inside weld,which are distinctly different from residual stress of the thin Ti-6Al-4V alloy plates presented in references before.  相似文献   

20.
Silicon carbide nanoparticle-reinforced nickel-based composites(Ni–Si CNP),with a Si CNPcontent ranged from1 to 3.5 wt%,were prepared using mechanical alloying and spark plasma sintering.In addition,unreinforced pure nickel samples were also prepared for comparative purposes.To characterize the microstructural properties of both the unreinforced pure nickel and the Ni–Si CNPcomposites transmission electron microscopy(TEM) was used,while their mechanical behavior was investigated using the Vickers pyramid method for hardness measurements and a universal tensile testing machine for tensile tests.TEM results showed an array of dislocation lines decorated in the sintered pure nickel sample,whereas,for the Ni–Si CNPcomposites,the presence of nano-dispersed Si CNPand twinning crystals was observed.These homogeneously distributed Si CNPwere found located either within the matrix,between twins or on grain boundaries.For the Ni–Si CNPcomposites,coerced coarsening of the Si CNPassembly occurred with increasing Si CNPcontent.Furthermore,the grain sizes of the Ni–Si CNPcomposites were much finer than that of the unreinforced pure nickel,which was considered to be due to the composite ball milling process.In all cases,the Ni–Si CNPcomposites showed higher strengths and hardness values than the unreinforced pure nickel,likely due to a combination of dispersion strengthening(Orowan effects) and particle strengthening(Hall–Petch effects).For the Ni–Si CNPcomposites,the strength increased initially and then decreased as a function of Si CNPcontent,whereas their elongation percentages decreased linearly.Compared to all materials tested,the Ni–Si CNPcomposite containing 1.5% Si C was found more superior considering both their strength and plastic properties.  相似文献   

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