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1.
Fe78B13Si9熔体与铁的润湿行为   总被引:1,自引:0,他引:1  
采用座滴法研究了真空条件下1 180~1 220℃之间Fe78B13Si9熔体在纯铁上的润湿行为,结合DeGennes液滴润湿动力学模型分析了Fe78B13Si9熔体在纯铁上的润湿动力学。结果表明:Fe78B13Si9熔体与铁间有良好的润湿性,平衡接触角在10°~40°之间;Fe78B13Si9熔体与铁的润湿为反应性润湿,润湿过程中由于熔体与基体之间的溶解和相互扩散,熔体体积首先增大,然后随着熔体等温凝固的进行又逐渐减小;由于熔滴体积在润湿过程中不断变化,以及测量接触角与实际接触角的差异,De Gennes液滴润湿动力学模型不能描述Fe78B13Si9熔体在铁基体上的铺展规律。  相似文献   

2.
采用单辊法制备了宽20 mm、厚25μm的Fe78Si9B13非晶带材,再将非晶带材进行不同温度的退火处理,研究了退火温度对其软磁性能的影响。结果表明,随退火温度的升高,Fe78Si9B13非晶带材的初始磁导率、饱和磁感应强度、矫顽力和电感呈先增大后减小的趋势;当退火温度达到400℃时,其综合软磁性能最佳,初始磁导率为6.648 K,饱磁感应强度为1.517 T,矫顽力为15.73 A/m。当退火温度达到450℃时,其磁导率受磁场强度的影响很小,呈现出恒导磁特性。  相似文献   

3.
采用动态电脉冲纵向磁场退火法,对Fe78B13Si9非品合金条带实施连续快速退火.测定了该合金条带的应力松弛、退火脆化及软磁性能随动态脉冲加热工艺参数的变化规律.试验结果表明,适当的动态脉冲加热工艺参数的配合,可以使Fe78B13Si9非晶合金条带的液淬内应力基本上完全松弛,磁性能优于最佳常规退火处理的条带性能,同时也完全消除了退火脆化现象.  相似文献   

4.
部分晶化法是一种具有实用前景的Fe78Si9B13非晶合金热处理方法。研究了不同热处理温度、热处理时间、保护气氛及冷却速度对Fe78Si9B13非晶合金磁性能的影响,探讨了获得具有一定恒导磁性能Fe78Si9B13非晶合金磁芯的方法。随热处理温度的上升,Fe78Si9B13非晶磁芯0A下的电感量单调下降,1A下的电感量先上升后下降。在一定保温温度和保护气氛下,随热处理时间的延长,Fe78Si9B13非晶磁芯0A下电感量单调减小,1A下电感量单调增加。较低的保温温度有利于在较宽保护气氛下获得所需磁性能的磁芯,过高真空度不利于获得所需的磁芯性能。不同冷却速度对Fe78Si9B13非晶磁芯电感量没有明显影响。  相似文献   

5.
室温下,对非晶Fe78Si9B13条带进行压力处理,通过不同的实验手段检测其热性能和耐腐蚀性能。XRD和热膨胀数据显示经过压力处理后Fe78Si9B13条带仍保持非晶状态,并且其内部自由体积数量随着压力的增加而单调增加。在10MPa的压力条件下非晶条带在不同溶液中的耐腐蚀性能减弱,在20MPa的压力条件下耐蚀性能增强,这种非线性变化与电阻率变化结果一致。可以通过由于压力引入样品中而导致自由体积的数量和硅原子的偏析来解释这一非单调变化。  相似文献   

6.
Fe78-2xCrxMoxSn2P10Si4B4C2(x=2,4)块体非晶合金的制备和性能   总被引:4,自引:2,他引:2  
本文用铜模上吸铸法制备Fe78-2xCrxMoxSn2P10Si4B4C2(x=2,4,原子百分比)块体非晶合金系列,制备出直径达2.5mm的Fe74Cr2Mo2Sn2P10Si4B4C2非晶合金棒材和直径达2mm的Fe74Cr2Mo2Sn2P10Si4B4C2非晶合金棒材。发现Fe74Cr2Mo2Sn2P10Si4B4C2具有32K的超冷液相区和高达0.61的约化玻璃转变温度,具有很强的玻璃形成能力。当x=2和x=4时非晶合金的居里温度分别为538K和455K,饱和磁感应强度分别为1.06T和0.71T。  相似文献   

7.
对退火Fe78Si9B13非晶合金部分晶化后的恒导磁特性进行了研究.结果表明,对于Fe78Si9B13非晶态铁基合金,随着退火温度的升高和退火时间的延长,晶化相逐渐增多.在适当温度经一定的时间退火后,初始磁导率和最大磁导率均逐渐减小,磁化曲线呈现出一定的线性关系,即合金呈现恒导磁特性.这种特性是由于表面晶化引起的体积收缩,给内部未晶化层施加了压应力,导致内部的磁畴横向排列,使合金产生恒导磁现象.  相似文献   

8.
研究了高温氧化对铁基非晶Fe78Si9B13合金软磁性能的影响。结果表明:非晶Fe78Si9B13合金带材经高温氧化处理后,在其表面形成了一层厚度约为10μm的高电阻率铁的氧化物层;Fe78Si9B13合金高温氧化磁化变得困难,且饱和磁感应强度Bs由氧化前的Bs=1.42~1.46 T下降到氧化后的Bs=1.29~1.38 T。同时,对非晶Fe78Si9B13合金带材经高温氧化处理后磁化困难的原因进行了讨论。  相似文献   

9.
研究了高温氧化对铁基非晶Fe78Si9B13合金软磁性能的影响。结果表明:非晶Fe78Si9B13合金带材经高温氧化处理后,在其表面形成了一层厚度约为10μm的高电阻率铁的氧化物层;Fe78Si9B13合金高温氧化磁化变得困难,且饱和磁感应强度Bs由氧化前的Bs=1.42~1.46 T下降到氧化后的Bs=1.29~1.38 T。同时,对非晶Fe78Si9B13合金带材经高温氧化处理后磁化困难的原因进行了讨论。  相似文献   

10.
介绍了基线修正法在采用差示扫描量热法(DSC)分析Fe基非晶合金Fe78Si9B13晶化动力学研究中的应用。充分考虑系统误差信号可能带来的影响,通过采用基线修正法得到各条DSC热分析曲线,在计算峰面积时,对晶化峰进行合适的切线修正,提高了峰面积及晶化率a计算结果的准确性。再根据Kissinger模型,计算了Fe78Si9B13非晶合金α-Fe相晶化过程的晶化激活能Ea为362 k J/mol。以此为基础,计算了对应的动力学指数n为1.5~2.0。Fe78Si9B13非晶合金的α-Fe相晶化过程是一个二维扩散控制的形核与长大过程。  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.
吴玉梅  熊晓云  靳蓉  孙敬民  杨林  罗晓星 《金属学报》2005,10(10):1100-1103
目的: 观察本实验室合成的一种治疗阿尔茨海默氏症(AD)的药物(1-二甲基磷酰基-2, 2, 2 -三氯)-乙基-1-醇烟酸醋(NMF),对体外培养的皮层神经细胞活性的影响以及对海人藻酸(KA)所致的神经损伤的保护作用。方法: 采用体外培养皮层神经元的方法,解剖分离 15 d胚胎小鼠皮层神经细胞, 接种于 96孔板,48 h 后加药并培养 72 h,以 MIT 法 观察 NMF 对小鼠皮层神经细胞活性的影响;同时将接种于 24 孔板的细胞预先给予 NMF,d 3 时加或不加KA处理后,以台盼蓝染色鉴别并计数死、活细胞,可得出细胞的存活率。结果: NMF 明显促进胎鼠皮层神经元活性,其中 NMF1、0. 1、10nmol·L-1促进神经元活性增殖率分别高达 34.7%、37.4%、36. 7%, NMF 明显促进正常胎鼠皮层神经元存活卒,与对照组比较,10nmol·L-1 NMF 对皮层神经元的存活率分别提高 39.3%、73.5%。 NMF能显著 对抗 KA 所致的神经元损伤,与 KA 损伤组相比, NMF0.1、10、10nmol·L-1对损伤皮层神经元的保护率分别为 77.30%、80.10%、84.15%。结论: NMF 明 显促进胎鼠皮层神经元的洁性、提高正常皮层神经元,的存活卒,并能有效地保护KA所致的神经元损伤,提示 NMF 是一种很有潜力的治疗 AD 的药物。  相似文献   

16.
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   

17.
Coherent second phase often exhibits anisotropic morphology with specifi c orientations with respect to both the second and the matrix phases. As a key feature of microstructure, the morphology of the coherent particles is essential for understanding the second-phase strengthening eff ect in various industrial alloys. This letter reports anisotropic growth of coherent ferrite from austenite matrix in pure iron based on molecular dynamics simulation. We found that the ferrite grain tends to grow into an elongated plate-like shape, independent of its initial confi guration. The fi nal shape of the ferrite is closely related to the misfi t between the two phases, with the longest direction and the broad facet of the plate being, respectively, consistent with the best matching direction and the best matching plane calculated via the Burgers vector content(BVC) method. The strain energy calculation in the framework of Eshelby's inclusion theory verifi es that the simulated orientation of the coherent ferrite is energetically favorable. It is anticipated that the BVC method will be applicable in analysis of anisotropic growth and morphology of coherent second phase in other phase transformation systems.  相似文献   

18.
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   

19.
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   

20.
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   

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