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1.
研究了在脉冲等离子体稀土渗氮过程中稀土元素La对氮浓度分布和相结构的影响,揭示了La在化合物层中的扩散规律,结果表明:与常规离子渗氮相比稀土绵添加,提高了表面氮浓度,随处理时间的延长而增加,当渗氮时间从2h增加至24h时,化合物导上ε-Fe2-3N(ε)转化为ε-Fe2-3N和γ‘-Fe4N(γ’)双相,此外,La可以扩散进入ε和γ‘相中,La的扩散规律受制于化合物的γ’-Fe4N的比例,随时间延  相似文献   

2.
离子束辅助沉积Fe-N薄膜的相形成SCIEI   总被引:1,自引:0,他引:1  
江海  武庆兰 《金属学报》1994,30(6):B273-B276
用离子束辅助沉积方法合成Fe-N薄膜,用离子束背散射和X射线衍射方法分析薄膜成分和结构.结果表明,薄膜的组分(α-Fe,ζ-Fe2N,ε-Fe(2-3)N,γ'-Fe4N相等)取决于沉积参数。给出了沉积温度和N/Fe原子到达比组成的相区域图.  相似文献   

3.
江海  武庆兰  陶琨  李恒德 《金属学报》1994,30(18):273-276
用离子束辅助沉积方法合成Fe-N薄膜,用离子束背散射和X射线衍射方法分析薄膜成分和结构.结果表明,薄膜的组分(α-Fe,ζ-Fe2N,ε-Fe(2-3)N,γ'-Fe4N相等)取决于沉积参数。给出了沉积温度和N/Fe原子到达比组成的相区域图.  相似文献   

4.
采用纯铁片渗氮,淬火及低温回火制得了含有α″-Fe16N2,γ′-Fe4N,含氮马氏体以及残余奥氏体等不同组分的Fe-N薄片。利用显微硬度计,X射线衍射仪及透射电镜分析了含氮马氏体在不同温度下的时效过程以及亚稳氮化物,α″-Fe16N2相的析出特征。  相似文献   

5.
采用电子衍射方法对Fe-1.83C马氏体室温时效时产生的有序相结构进行研究,确定其结构为偏离化学计量成分Fe_4C的γ′-Fe_4结构,称为γ′-Fe_xC(Ⅰ)(x=4-11)。碳原子位于单胞的1/2,1/2,1/2位置。该有序相单胞尺寸为:(a_M,c_M分别为马氏体单胞的a和c轴长度),它与母相完全共格,位向关系为(001)_Ⅰ∥(001)_M,[100]_Ⅰ∥[110]_M。根据γ′-Fe_xC(Ⅰ)晶体结构计算出的有序相衍射花样与实验得到的衍射花样全部吻合。  相似文献   

6.
采用电子衍射方法对Fe-1.83C马氏体室温时效时产生的有序相结构进行研究,确定其结构为偏离化学计量成分Fe_4C的γ′-Fe_4结构,称为γ′-Fe_xC(Ⅰ)(x=4-11)。碳原子位于单胞的1/2,1/2,1/2位置。该有序相单胞尺寸为:(a_M,c_M分别为马氏体单胞的a和c轴长度),它与母相完全共格,位向关系为(001)_Ⅰ∥(001)_M,[100]_Ⅰ∥[110]_M。根据γ′-Fe_xC(Ⅰ)晶体结构计算出的有序相衍射花样与实验得到的衍射花样全部吻合。  相似文献   

7.
任晓兵  清水谦一 《金属学报》1994,30(7):A296-A301
采用电子衍射方法对Fe-1.83C马氏体室温时效时产生的有序相结构进行研究,确定其结构为偏离化学计量成分Fe_4C的γ′-Fe_4结构,称为γ′-Fe_xC(Ⅰ)(x=4-11)。碳原子位于单胞的1/2,1/2,1/2位置。该有序相单胞尺寸为:(a_M,c_M分别为马氏体单胞的a和c轴长度),它与母相完全共格,位向关系为(001)_Ⅰ∥(001)_M,[100]_Ⅰ∥[110]_M。根据γ′-Fe_xC(Ⅰ)晶体结构计算出的有序相衍射花样与实验得到的衍射花样全部吻合。  相似文献   

8.
用磁控溅射技术成功的制备了Fe-N/Ti-N纳米多层膜.Fe-N层厚度固定为2.2nm,Ti-N层厚度在0.5nm和4.6nm之间依次变化.由X射线衍射结果发现样品中有Fe16N2相存在,发现Ti-N层厚度的变化,对剩磁比、饱和外场、矫顽力、饱和磁化强度(MS)有很大影响,Fe-N层之间有铁磁耦合和反铁磁耦合变化.  相似文献   

9.
王合英  姜恩永  白海力  吴萍  刘明升 《金属学报》1996,32(11):1199-1203
用对向靶溅射仪制备出含多量Fe(16)N2相的(Fe,Ti)-N薄膜,研究了掺杂Ti对Fe-N薄膜结构与磁性的影响,在溅射Fe-N薄膜时加入适量的Ti可提高Fe-N薄膜中Fe(16)N2相的含量.Ti含量(原子分数)在0—25%时薄膜饱和磁化强度均高于纯Fe的值;Ti浓度为10%时,薄膜磁化强度高达2.68T,比纯Fe的饱和磁化强度值高20%.  相似文献   

10.
用对向靶溅射仪制备出含多量Fe(16)N2相的(Fe,Ti)-N薄膜,研究了掺杂Ti对Fe-N薄膜结构与磁性的影响,在溅射Fe-N薄膜时加入适量的Ti可提高Fe-N薄膜中Fe(16)N2相的含量.Ti含量(原子分数)在0—25%时薄膜饱和磁化强度均高于纯Fe的值;Ti浓度为10%时,薄膜磁化强度高达2.68T,比纯Fe的饱和磁化强度值高20%.  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.
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   

18.
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   

19.
A new method was introduced to achieve directional growth of Sn crystals. Microstructures in liquid(Pb)/liquid(Sn) diffusion couples were investigated under various static magnetic fields. Results show that the β-Sn crystals mainly reveal an irregular dendritic morphology without or with a relatively low static magnetic field(B0.3 T). When the magnetic field is increased to 0.5 T, the β-Sn dendrites close to the final stage of growth begin to show some directional character. With a further increase in the magnetic field to a higher level(0.8–5 T), the β-Sn dendrites have an enhanced directional growth character, but the dendrites show a certain deflection. As the magnetic field is increased to 12 T, the directional growth of the β-Sn dendrites in the center of the couple is severely destroyed. The mechanism of the directional growth of the β-Sn crystals and the deflection of the β-Sn crystals with the application of static magnetic field was tentatively discussed.  相似文献   

20.
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   

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