电沉积工艺参数对镍-钼-锌三元合金电极析氢催化性能的影响

目的采用直流电沉积法在铜基底上制备镍-钼-锌三元合金电极,提高电解水析氢过程中阴极电极的效率。方法使用电化学工作站研究不同电沉积工艺参数对镍-钼-锌三元合金镀层析氢性能的影响,使用扫描电镜(SEM)、X射线衍射分析仪(XRD)、能谱仪(EDS)对合金镀层表面形貌、相结构及元素含量进行表征。通过线性扫描伏安法(LSV)对析氢过电位进行测量,采用塔菲尔极化获得塔菲尔斜率,采用电化学阻抗法(EIS)表征合金镀层的析氢催化性能。结果最佳工艺参数为:温度45℃,p H=10.5,电流密度100 mA/cm~2。该合金在10 mA/cm~2下相对氢标电位仅为139 mV,塔菲尔斜率为103 mV/dec,活化电极电阻(Rct)随着电压的升高而降低。合金中Ni、Mo和Zn的原子比分别为68.23%、10.09%和21.68%。合金镀层为非晶结构,表面是纳米级颗粒堆叠而成的粗糙形貌。结论不同的工艺参数对Ni-Mo-Zn电极析氢性能有着重大影响,其析氢性能随着p H值的升高而上升,随着电流密度的升高而先增后减,随着电沉积温度的升高而上升。Ni-Mo-Zn高的析氢性能源于其元素协同作用、非晶结构和粗糙表面。     

电沉积非晶/纳米晶Ni-Mo-La合金电极的析氢性能

在非晶/纳米晶Ni-Mo合金镀液中添加适量的LaCl3溶液,获得了非晶/纳米晶混合结构的Ni-Mo-La合金电极。结果表明:稀土La元素的加入,有利于镀层Mo含量的提高,形成非晶态Ni-Mo合金,细化镀层晶粒,减小镀层微应变,并使镀层表面积增加。在25℃、7 mol/L的NaOH溶液中的电化学实验表明:Ni-Mo-La合金电极比Ni-Mo合金电极具有更高的析氢催化活性,在电流密度为150 mA/cm2条件下,Ni-Mo-La合金电极的析氢过电位比Ni-Mo合金电极的降低了约80 mV。Ni-Mo-La合金具有储氢材料的特性,其析氢过程含有吸氢—储氢—脱附的过程。     

钛基Ni-Co-P非晶合金镀层电极的析氢性能

通过电沉积在钛基体上制备了非晶态Ni-Co-P合金镀层.在7mol/L NaOH溶液中进行的电化学测试结果表明,Ni-Co-P合金电极的析氢过电位明显低于镀镍阴极和纯钛阴极;计算了电极析氢反应的电化学动力学参数,表明非晶态Ni-Co-P合金电极具有较好的析氢电催化活性.     

钛基镍钴合金电极的制备及析氢性能

目的降低电极的析氢过电位,提高析氢性能,从而降低电解水制氢的成本,促进氢储能技术的发展。方法通过异相共沉积法,制备了镍钴合金电极。利用场发射扫描电镜(SEM)、电化学交流阻抗(EIS)对纯镍电极及镍钴合金电极进行表征,采用阴极极化曲线(LSV)探究了电沉积液中Ni/Co元素的比例、电沉积电位及电沉积时间对镍钴合金电极析氢性能的影响。结果 SEM结果揭示了纯镍电极及镍钴合金电极表面分别是粒径约为100 nm左右的镍颗粒和镍钴颗粒。EIS结果说明了镍钴合金电极的导电性能优于纯镍电极。此外,纯镍电极、镍钴合金电极的阴极极化曲线测试表明在电流密度为30 mA/cm~2时,镍钴合金电极的析氢过电位比纯镍电极降低55 mV,降低了近20%。结论通过异相共沉积法制备镍钴合金电极,制备方法简单、方便、快速,其析氢性能优于纯镍电极。镍钴合金电极的最优制备工艺条件为:NiSO_4·6H_2O 27 g/L,CoSO_4·7H_2O_3 g/L,H_3BO_3 10 g/L,Na_2SO_4 10 g/L,柠檬酸10 g/L,十二烷基硫酸钠0.1 g/L,pH值4.0,电沉积电位-1.3 V,电沉积时间10 s。     

纳米多孔NiFeCoTi高熵合金电极的析氢反应性能

开发高效、稳定的电催化剂用于电化学水分解制氢至关重要。通过合金化和脱合金化法制备了纳米多孔NiFeCoTi高熵合金电极,并对其碱性析氢反应性能进行了研究。结果表明：该电极具有柱状纳米多孔结构,能够促进电催化反应过程中的电子传递和质量运输,表面的NiFeCoTi高熵合金可以提供双功能的电催化活性位点,促进水的解离和氢中间体的吸附/结合。在1 M KOH电解液中,纳米多孔NiFeCoTi电极在～111 mV的过电位下就能够达到400 mA/cm²的电流密度,具有较低的Tafel斜率和优异的长期稳定性。     

一步电沉积法制备Ni-Mo-Nd/NF复合电极及其析氢性能研究

目的 采用一步恒电流沉积法在泡沫镍基底上制备出镍-钼-钕三元析氢电极,提高碱性条件下的析氢性能。方法 使用电化学工作站研究工艺参数对Ni-Mo-Nd/NF析氢电极性能的影响,同时制备Ni-Mo/NF析氢电极,使用扫描电镜(SEM)、X射线衍射分析仪(XRD)、能谱仪(EDS)和X射线光电子能谱(XPS)对合金镀层表面形貌、相结构、元素含量及成键状态进行表征。通过线性扫描伏安法(LSV)、循环伏安法(CV)及电化学阻抗技术(EIS)测试电极析氢性能。结果 最佳工艺参数为:pH=4.5,电流密度30 mA/cm²,沉积时间60 min,温度30 ℃。在1.0 mol/L KOH溶液中,Ni-Mo-Nd/NF电极在10 mA/cm²下的析氢过电位仅为73 mV,Tafel斜率为147 mV/dec,表明析氢反应机理遵循典型的Volmer-Heyrovsky步骤。此外,Ni-Mo-Nd/NF电极在长时电解24 h时电流密度保持稳定,2 000次循环伏安测试后,催化剂的活性衰减微小。结论 稀土元素Nd的掺杂,能够细化电极表面的球形颗粒并提高电极表面粗糙度,从而提升电极的比表面积,为析氢反应提供更多的活性位点,利于析氢反应效率的提高。由于三元合金的协同作用,与二元合金Ni-Mo/NF相比,Ni-Mo-Nd/NF三元合金电极显示出更优异的HER催化性能。     

添加剂Pr2O3和Er2O3对电沉积Ni-S合金电极性能的影响

以氧化镨、氧化铒为添加剂,在泡沫镍基体上电沉积制备Ni-S镀层电极。对镀层的表面形貌、镀层结构、电沉积行为及镀层的电化学性能进行研究。结果表明：电镀液中添加稀土氧化物后电沉积过程的阴极极化增强,沉积层晶粒细化,比表面积增大,因而电极的析氢过电位降低;其中,添加Pr203的Ni-S镀层在250mA／cm2下碱性水电解时过电位降低达37mV,且该镀层电极在碱性介质下具有较高的析氢活性和耐腐蚀性能,在100h水电解实验中表现出较强的稳定性。     

Hydrogen Evolution Reaction of the Electrodeposited Amorphous Ni--S—Co Alloy in Alkaline Medium

通过电沉积方法获得了Ni-S-Co非晶合金镀层．电化学测试结果表明，非晶态Ni-S-Co合金电极的析氢过电位仅为70mV，析氢反应的电化学活性高于其它种类的电极(包括非晶态Ni-S合金电极)，计算了电极的电化学参数(Tafel斜率b,交换电流密度i0和表观活化能△H^*)．XRD和SEM测试表明，在电解过程中，非晶态Ni-S-Co合金电极的电化学稳定性高于非晶态Ni-S合金电极．长时间电解实验表明，非晶态Ni-S-Co合金电极在模拟工业电解条件下具有相当高的活性和稳定性．     

泡沫基材-Ni-石墨烯复合镀层制备及电催化析氢性能研究

目的 采用电沉积技术在泡沫基材上沉积制备Ni-石墨烯复合镀层,期望借助泡沫基材的三维多孔结构和石墨烯的超高比表面积来改变复合材料的表面状态,进而获得高镀层的电催化析氢性能。方法 采用电沉积技术将石墨烯作为第二相粒子沉积,制备了泡沫基材-Ni-石墨烯复合电极,通过SEM和EDS研究了其微观形貌及成分,并利用电化学工作站完成了镀层电极的极化曲线、交流阻抗和电解水稳定性测试,使用控制变量法探究了镀层厚度、镀液石墨烯浓度和基材形貌对镀层电催化析氢活性的影响。结果 SEM和EDS表征发现,镀层表面形貌受镀液中石墨烯浓度影响较大,石墨烯作为第二相嵌入镀层后,明显改变了复合镀层的表面形貌,其存在形态为颗粒状,在150 mg·L^–1时颗粒堆积最多。进一步利用电化学分析技术探究了镀层厚度、镀液石墨烯浓度和基材形貌对电极电催化析氢性能的影响,发现在一定范围内,不同厚度镀层的电催化析氢活性基本相同;石墨烯质量浓度为150mg·L^–1时制得的电极的电催化析氢性能最优,析氢过电位为211.2m V(vs.RHE),且电解水稳定性良好;泡沫基材镀层的电催化析氢活性明显优...     

不同搅拌方式对Ni-Fe-Co镀层组织结构和电催化析氢性能的影响

目的得到具有更高电催化析氢活性的Ni-Fe-Co镀层电极。方法采用不同的搅拌方式电沉积制备了Ni-Fe-Co镀层,通过SEM、EDS和XRD等分析手段研究了其微观形貌、成分及物相组成,并利用电化学测试分析技术探究了不同搅拌方式对其电催化析氢活性的影响。结果三种镀层电极均为简单固溶体BCC结构,其中磁力搅拌条件下制得的镀层电极的表面组织更致密均匀,具有更大的真实表面积,分别为不搅拌和超声搅拌下的6倍和2倍。在电位为-1.6 V时,磁力搅拌条件下制得的镀层电极析氢电流密度达到173m A/cm~2,明显高于另外两种镀层电极,其交流电流密度为45.9μA/cm~2,分别是不搅拌和超声搅拌条件下的2倍和3倍。结论磁力搅拌有效地增大了镀层的比表面积,进而提高了镀层的电催化析氢活性。     

Effects of Post-weld Heat Treatment on Microstructure,Mechanical Properties and the Role of Weld Reinforcement in 2219 Aluminum Alloy TIG-Welded Joints

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.     

The First Phase of the SRIF Industrialized Base in ＂West Area＂ Has Been Put into Operation

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.     

THERMODYNAMICS STUDY ON THE DECOMPOSITION OF CHROMITE WITH KOH

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.     

INFLUENCE OF HEAT TREATMENT ON DAMPING BEHAVIOUR OF THE MAGNESIUM WROUGHT ALLOY AZ61

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.     

新型的治疗阿尔茨海默氏症药物(1-二甲基磷酰基-2,2,2-三氯)-乙基-1-醇烟酸醋对体外神经细胞的作用

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。     

Effect of Rare Earth Doping on Impedance,Modulus and Conductivity Properties of Multiferroic Composites:0.5(BiLa_xFe_(1-x)O_3)–0.5(PbTiO_3)

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).     

Three-Dimensional Growth of Coherent Ferrite in Austenite: A Molecular Dynamics Study

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.     

Using Finite Element and Contour Method to Evaluate Residual Stress in Thick Ti-6Al-4V Alloy Welded by Electron Beam Welding

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.     

Microstructures and Tensile Properties of Ultrafine-Grained Ni–(1–3.5) wt% SiC_(NP) Composites Prepared by a Powder Metallurgy Route

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.     

Directional Growth of Tin Crystals Controlled by Combined Solute Concentration Gradient Field and Static Magnetic Field

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.