Effect of different deformation and annealing procedures on non-magnetic textured Cu<Subscript>60</Subscript>Ni<Subscript>40</Subscript> alloy substrates

In this work, a series of specimens was prepared by the casting method. Sharp cube-textured substrates were processed by heavy cold rolling and recrystallization annealing (i.e., the rolling-assisted biaxially textured substrates (RABiTS) method). Both the rolling and the recrystallization texture in the alloy tapes were investigated by X-ray diffraction and electron back-scatter diffraction, respectively. The results showed that a strong copper-type deformation texture was obtained in the heavy cold-rolled substrate. In addition, the recrystallization annealing process was found to be very important for the texture transition in the Cu–Ni alloy substrates. The cube texture content in the Cu₆₀Ni₄₀ alloy substrates reached 99.7% (≤10°) after optimization of the cold-rolling procedure and the recrystallizing heat-treatment process, whereas the content of low-angle grain boundaries (from 2° to 10° misorientation) in the substrate reached 95.1%.     

时效处理对Ti50Ni25Cu25合金阻尼行为的影响

采用内耗测试和Ｘ－射线衍射研究了时效处理对Ｔｉ５０Ｎｉ２５Ｃｕ２５合金阻尼特性的影响,发现随时效温度升高,相变内耗峰降低,并且出现Ｂ１９’马氏体,低温时效合金背底内耗随振动频率增大而降低,高温时效合金背底内耗与振动频率无关。     

Glass-forming ability,microhardness, corrosion resistance,and dealloying treatment of Mg_(60-x)Cu_(40)Nd_x alloy ribbons

The influence of Nd addition on the glass-forming ability(GFA), microhardness, and corrosion resistance of Mg_(60-x)Cu_(40)Nd_x(x = 5, 10, 15, 20, and 25, at%) alloys were investigated by differential scanning calorimetry, Vickers-type hardness tests, and electrochemical methods. The results suggest that the GFA and microhardness of the amorphous alloys increase until the Nd content reaches 20at%. The corrosion potential and corrosion current density obtained from the Tafel curves indicate that the Mg_(35)Cu_(40)Nd_(25) ternary alloy exhibits the best corrosion resistance among the investigated alloys. Notably, nanoporous copper(NPC) was synthesized through a single-step dealloying of Mg_(60-x)Cu_(40)Nd_x(x = 5, 10, 15, 20, and 25) ternary alloys in 0.04 mol·L~(-1) H_2SO_4 solution under free corrosion conditions. The influence of dealloying process parameters, such as dealloying time and temperature, on the microstructure of the ribbons was also studied using the surface diffusivity theory. The formation mechanism of dealloyed samples with a multilayered structure was also discussed.     

Cu_(73)Sn_6Ni_6P_(15)非晶的微观结构和驰豫过程

用X射线衍射方法测定了Cu_(73)Sn_6Ni_6P_(15)非晶的结构参数,利用电阻法对其结构驰豫过程进行了研究,并给出了结构驰豫激活能。     

稀土Er对ZK60镁合金变形行为的影响

采用Gleeble-1500D热模拟试验机研究了稀土元素Er对ZK60镁合金的热压缩变形行为的影响。通过引入Zener-Hollomon参数和双曲正弦函数构建了ZK60和ZK60-1.0Er镁合金的本构方程,同时采用应变硬化率θ-流变应力σ关系曲线确定动态再结晶发生的临界应力σc值。结果表明:ZK60和ZK60-1.0Er两种镁合金在热压缩变形过程中,随着变形温度T的升高,压缩流变应力σ值均减小;随着应变速率ε?的增加,流变应力σ值均增加。添加稀土元素Er使得ZK60镁合金热压缩变形流变应力σ值和应力指数n值增加,在变形温度为160~320℃时提高了发生动态再结晶的临界应力σc值,稀土相的存在促进了再结晶晶粒的形核,降低了平均变形激活能Qˉ值。     

Zr_(55)Al_(10)Ni_5Cu_(30)大块金属玻璃的晶化行为研究

分别在603 K、653 K、683 K、723 K、753 K、793 K和0.5 h、1 h、2 h、3 h、5 h的保温时间下对Zr55Al10Ni5Cu30大块金属玻璃进行了退火热处理.采用x射线衍射(XRD)法分析了退火后Zr55Al10Ni5Cu30大块金属玻璃的弛豫和晶化相析出的过程,计算了不同温度下结晶度和纳米晶粒尺寸的大小.通过差示扫描量热(DSC)法分析了Zr55Al10Ni5Cu30大块金属玻璃的热稳定性.Kjssinger曲线分析表明,Zr55Al10Ni5Cu30大块金属玻璃弛豫后晶化激活能高于其淬态的晶化激活能,退火温度对大块金属玻璃热稳定性有显著影响.     

Fe对Zr_(55)Al_(10)Ni_5Cu_(30)非晶形成能力及力学性能的影响

为了进一步提高锆基大块非晶合金的玻璃形成能力及力学性能,采用铜模吹铸法制备了(Zr0.55Al0.10Ni0.05Cu0.30)100-XFeX(X=1,5,10)系列合金,通过X射线衍射(XRD)、差示扫描量热法(DSC)以及压缩实验和SEM进行材料分析。研究表明:微量Fe有助于改善非晶合金在压缩变形时剪切带内的应力分布,提高材料的综合性能,当Fe添加量为1%时,塑性应变εp达到5.9%,强度达到1.89GPa,同时,随着Fe添加量的增加,过冷温度区间△Tx减小,热稳定性减小,非晶形成能力降低。     

Ti_(62)Zr_(17)Cu_6Ni_(15)合金晶化实验分析

对Ti6 2 Zr1 7Cu6 Ni1 5非晶合金原始样品进行了退火晶化处理和激波晶化处理 ,对样品作了XRD分析并重点对样品进行了差示扫描量热分析 (DSC)以及动力学分析 .看到了许多有趣的现象并得到了一些有价值的动力学参数     

La0.5Sr0.5Ni0.5Cu0.5O3催化剂上的CO氧化反应动力学

利用内循环无梯度反应器对钙钛矿型催化剂 La0 .5 Sr0 .5 Ni0 .5 Cu0 .5 O3上 CO氧化反应的动力学进行了研究 ,实验中通过分别测定 CO和 O2 的分压对氧化反应速率的影响 ,得出了相应的曲线关系 ,通过对所有动力学数据用计算机进行多元线性回归 ,得出动力学方程 r =2 .2 6× 1 0 8e-1 0 3 0 0 0 /8.3 1 4 T Pco0 .5 ,根据动力学实验结果初步提出了 CO在该催化剂上氧化机理模型 .     

Effect of solution treatment on the martensitic transformation behavior of a Ni_(43)Co_7Mn_(39)Sn_(11) polycrystalline alloy

The effect of solution treatment on the martensitic transformation behavior of a Ni43Co7Mn39Sn11 polycrystalline alloy fabricated by an arc melting method was investigated by scanning electron microscopy(SEM), energy-dispersive X-ray spectroscopy(EDS), and differential scanning calorimetry(DSC). The examination indicates the presence of severe chemical segregation in the dendritic as-cast structure because of solidification. This chemical segregation completely impedes the intrinsic martensitic transformation. Annealing at 1223 K for 24 h is identified as the threshold annealing condition to eliminate the microstructural segregation and begin the martensitic transformation, as indicated by a broad and obscure feature. Annealing at 1273 K for 24–48 h is found to be effective at promoting notably the martensitic transformation, but the martensitic transformation exhibits a multiple-step feature. Complete homogeneity is achieved by annealing at 1273 K for 72 h, which produces a sharp, single-step martensitic transformation. The microstructural evolution and the valence electron concentrations of alloys(e/a ratio) are evaluated, which are reflective of the degree of compositional homogeneity of alloys, confirming that high annealing temperature and long holding time are vital to reveal the intrinsic martensitic behavior of this alloy. The adequately homogenized alloy displays a martensitic transformation at 292 K and an enthalpy of 11.2 J/g.     

非晶态合金Fe_(40)Co_(40)P_(20)局域结构及电子性质

利用密度泛函理论(DFT)方法,在B3LYP/Lanl2dz水平下,对原子簇Fe2Co2P中40种可能存在构型在二、四重态下进行全参数优化和频率验证,获得了18种稳定构型,分别对其能量、几何参数和电子性质进行了详细分析。结果显示:原子簇Fe2Co2P能够稳定存在的几何构型中既得到了单帽四面体和三角双锥的立体构型,又得到了五边形和菱形的平面构型;原子簇Fe2Co2P中金属和类金属之间的成键立体构型强于平面构型,立体构型中成键主要是由金属和类金属提供的,平面构型中金属与类金属之间及金属与金属之间对成键的影响相差不大;从电子性质得出影响因素主要是几何构型及金属与类金属的成键数目,P所带相对电荷量与其周围成键金属原子数成正比。     

轧制对Zr60Al15Ni25块体非晶合金晶化动力学的影响

通过线性DSC实验研究了轧制对Zr60Al15Ni25大块非晶合金晶化动力学的影响。实验结果表明,Zr60Al15Ni25非晶合金在轧制塑性变形过程中,随着变形量的增加,热稳定性降低。Zr60Al15Ni25块体非晶合金轧制后原子组态的变化主要影响晶化的形核阶段,变形量较低时(20%)合金原子组态向无序方向发展,导致晶化速率变慢,晶化变得比较困难。随着轧制的进一步增加,合金原子的无序性降低,晶化速率又逐渐提高,从而使其在随后加热过程中的晶化变得比较容易。     

变形参数对AZ31镁合金变形抗力的影响

利用Gleeble-1500热模拟试验机对AZ31镁合金在变形温度为250～400℃、变形速率为0.5～3.0s-1下进行热变形模拟实验,得到了AZ31镁合金真实应力-真实应变曲线,并通过光学显微镜观察了试样在变形中的微观组织.结果表明,动态再结晶是该实验条件下晶粒细化的主要机制,变形参数影响了再结晶的程度.     

LaMn_(7.2)Ni_(4.8)和LaMn_(8.4)Ni_(3.6)磁化率的研究

合成了稀土元素——过渡族元素化合物LaMn_(7.2)Ni_(4.8)和LaMn_(8.4)Ni_(3.6),并在77～302K温度范围内测量了它们在热处理前后的磁化率。实验表明合金LaMn_(7.2)Ni_(4.8)在热处理前的磁性质由Mn~( 2)离子决定,热处理后由Mn~( 2)离子和Ni~( 2)离子共同决定;LaMn_(8.4)Ni_(3.6)在热处理前呈泡利电子顺磁性,热处理后其磁性质由Ni~( 2)离子决定。     

Ni_(80)Fe_(20)镀层对Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9非晶条带磁阻抗效应的影响(英文)

采用磁控溅射镀膜工艺,在Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9非晶条带的光滑面上溅射了130~650 nm厚的Ni_(80)Fe_(20)薄膜,制备了一系列Ni_(80)Fe_(20)/Fe_(73.5)Cu_1Nb_3Si_(13.5)B_9复合结构样品.研究了镀层厚度对材料的镀层形貌、巨磁阻抗效应(Giant Magneto-Impedance,GMI)和磁滞回线的影响.结果发现,镀层厚度为260 nm厚时,样品的表面形貌最平整致密,最大磁阻抗比提高到33.0%.在玻璃基片上溅射了相同厚度的系列Ni_(80)Fe_(20)薄膜,其磁滞回线结果发现薄膜的各向异性方向随着厚度的增加由平行表面转变成垂直于表面.正是Ni_(80)Fe_(20)镀层各向异性的方向改变,影响了镀层与条带间的相互作用,进而影响复合结构样品的磁阻抗效应.     

Cu_(60)Zr_(29)Ti_(11)大块非晶合金的黏度特征和强液体行为

采用铜模铸造法制备了Cu60Zr29Ti11大块非晶合金,用X射线衍射仪、三点压弯式黏度仪对该非晶合金的动力学性质进行了研究.测定了大块非晶合金Cu60Zr29Ti11在过冷液相区的黏度,得到了它的动力学脆性系数m=31,以及流变激活能E=63.4kJ/mol.表明大块非晶合金Cu60Zr29Ti11是一种强液体,有较强的非晶形成能力,形成非晶比较稳定.分析了合金在过冷态的流变激活能变化规律,发现流变激活能的变化并不符合Kivelson的Super-Arrhenius公式.     

热处理对镍基合金涂层与基体结合界面的影响

通过热浸镀法在普碳钢表面成功制备镍基合金涂层.为了提高镍基合金涂层与钢基体之间的结合强度,对镀有镍基合金涂层的基体进行了热处理.研究了热处理前、后结合界面处的显微组织和力学性能.结果表明,与热处理前相比,热处理后界面附近的涂层中析出物长大,界面处存在不连续块状铁的硼化物,界面两侧镍、铁互扩散距离增加,靠近界面的过渡带由5～8μm变为20μm.热处理前、后涂层均由γ-(Fe,Ni)、CrB、Cr2B和Cr3C2等相组成,过渡带相组成为γ-(Fe,Ni)、微量CrB和Fe23(C,B)6.热处理后,显微硬度由界面向涂层内逐渐增加,界面结合强度由140MPa提高到200MPa.