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研究了新试剂2-[2′-(6′-甲氧基-苯并噻唑)偶氮]-5-二甲氨基苯甲酸(MOBTAMB)与Fe(Ⅱ),Ni(Ⅱ)的显色反应。在混合表面活性剂(TritonX-100-SDS)存在下,于pH5.2的HAc-NaAc缓冲溶液中,Fe(Ⅱ),Ni(Ⅱ)与MOBTAMB反应均形成1:2的稳定络合物。前者最大吸收波长为651nm,后者最大吸收波长为658nm。选定656nm为测定波长,测得表观摩尔吸光系数分别为ε_Fe-MOBTAMB=8.3×10 ̄4,ε_Ni-MOBTAMB=1.29×10 ̄5。铁浓度在0 相似文献
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在聚乙烯醇(PVAVA)存在下,铱与钼酸盐和罗丹明B(RB)形成离了缔合物。缔台物的最大吸收位于570nm摩尔吸光系数ε8.36×10 ̄5’L·mol ̄-1·cm ̄-1,服从比尔定率范围为0~2.75μglr/25ml。测定2.0μg铱的相对标准偏差为2.5%(n=7),检出限43n/ml(n=12)。测定铱的适宜条件为CHClO_4=0.93mol/L,C_MoO ̄2-_49.0×10~-4mol/L,C_RB=3.3×l0 ̄-5mol/L,PVAO08%。试验了30多种共存离子的影响,除形成杂多酸元素 相似文献
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2-(2-苯并噻唑偶氮)-5-磺丙氨基苯酚高效液相色谱法测定钢中钒、钴和镍 总被引:1,自引:0,他引:1
在KIO_4存在下,研究了2-(2-苯并噻唑偶氮)-5-磺丙氨基苯酚(BTASPAP)与V(Ⅴ),Co(Ⅱ)和Ni(Ⅱ)形成稳定络合物的反应,在Cl8柱上,以含0.2mol/L的乙酸-乙酸钠缓冲溶液(pH3.5)和1.0×10-3mol/L,溴化四丁基铵的乙腈-丙酮-水(36+1+63)为流动相洗脱液,在565nm处检测。V(Ⅴ),CD(Ⅱ)和Ni(Ⅱ)的络合物在6min内获得完全分离,检测限分别为15.0ng/ml,15.0ng/ml和40.0mg/ml.该方法已用于合金钢中钒、钴和镍的测定。 相似文献
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本文提出了一种新的光度测定论的方法。该方法基于在聚乙烯醇(PVA)存在下,钯与钼酸盐和丁基罗丹明B(BRB)反应形成离子缔合物。缔合物的最大吸收位于580nm,摩尔吸光系数ε为3.14×10 ̄5L·mol ̄(-1)·cm ̄(-1),钯量在0~4ug/25ml范围内服从比尔定律。缔合物中pd:BRB=1:4,体系至少可稳定10h,测定钯的适宜条件是:C_(HCO4)=1.6mol/L,C_(BRB)=3.8×10 ̄(-5)mol/L,PVA0.08%。考察了30多种共存离子的影响。本法用于碳基和铝基催化剂中 相似文献
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为了提高La-Mg-Ni基贮氢合金的荷电保持率,本文研究了La/Nd比的变化对La-Mg-Ni基贮氢合金自放电性能的影响。随着Nd替代La量的增加,(LaxNdy)0.9Mg0.10Ni3.09Mn0.12Co0.60Al0.13(x/y=5,4,3,2,1)合金的荷电保持率先增大后减小,当x/y=4时,其荷电保持率达到最大值80.8%(318 K)。合金电极贮存后,FESEM-EDS和XRD分析表明,合金颗粒表面形成了Mg(OH)2和Nd(OH)3。P-C-T曲线和Tafel极化测试表明,随着Nd含量的增加,金属氢化物的稳定性呈现先增加后降低和腐蚀电流先减小后增大的规律。 相似文献
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用磁控溅射方法制备了系列 (Fe0 .86 Zr0 .0 33Nb0 .0 33B0 .0 6 8Cu0 .0 1 ) x(Al2 O3) 1 -x颗粒膜样品 ,体积百分比x从 0 .3 3~ 0 .63 ,样品厚度约为10 0nm。室温下在Fe0 .86 Zr0 .0 33Nb0 .0 33B0 .0 6 8Cu0 .0 1 体积百分比x =0 .43时得到 17.5 μΩ·cm的最大饱和霍耳电阻率 ,比纯铁磁金属提高了 3~ 4个量级。对其磁性和微结构进行了研究 ,样品霍耳电阻率随外场的变化曲线 ρxy~H与磁场平行于膜面时的磁化曲线M~H有相似性 ,说明霍尔电阻率 ρxy与磁化强度M相关。样品电阻率 ρxx随金属体积百分比x的减小而增加 ,在x =0 .43附近发生突变 ,从金属导电变为绝缘体。根据微结构和输运性质对可能的机制进行了探讨 相似文献
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The room temperature creep behaviors of Mg61Cu28Gd11 and(Mg61Cu28Gd11)99.5Sb0.5 bulk metallic glasses(BMGs) were revealed by means of nanoindentation technique.The creep mechanism was explored by characterization of creep rate sensitivity,creep compliance and retardation spectra.The results showed that the experimental creep curves could be well described by a generalized Kelvin model.The low creep rate sensitivity of both Mg-based BMGs indicated that their room temperature creep was dominated by localized shear flow.In addition,the(Mg61Cu28Gd11)99.5Sb0.5 glassy alloy exhibited lower creep rate sensitivity,creep compliance and milder retardation peak,indicating its higher creep-resistance and less relaxed state.Furthermore,the creep retardation spectrum consisted of two relatively separated peaks with the well defined characteristic relaxation times. 相似文献
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使用电弧熔炼法制备了La1.1Fe11.4Si1.55Ge0.05合金。研究了用少量的Ge替代Si后,La1.1Fe11.4Si1.55Ge0.05合金的磁性和磁热效应。粉末X射线衍射结果表明:在1273K真空退火处理10d后,合金La1.1Fe11.4Si1.55Ge0.05主相为NaZn13型立方结构,存在微量的α-Fe相。热磁曲线M-T与Arrott曲线表明:在居里温度Tc=205K处发生由铁磁性(TTc)转变为顺磁性(TTc)的二级磁相变。在磁场变化0~1.5T下,根据等温磁化曲线通过Maxwell关系式计算得出最大磁熵变-ΔSmmax=9J.kg-.1K-1。Ge替代Si后该合金在其居里温度Tc处-ΔSm-T曲线半高宽增大,使合金的相对制冷能力RCP(S)有所提高。 相似文献
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InrecentyearsThMn12 typeiron richcompoundshavebeenintensivelyinvestigatedduetotheirexcellentpermanent magneticproperties .AlthoughpurebinaryRE Fecom poundsdonotexist,theThMn12 structurecanbestabilizedinpseudobinariesofthetypeREFe12 -xMx,withM =Al,Ti,Cr ,Si ,Mo ,V … 相似文献
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KineticsofHydrogenAbsorptioninMmNi_(3.55)Co_(0.75)Mn_(0.4)Al_(0.3)AlloyLinQin(林勤),YuZhentao(于振涛),YeWen(叶文)(UniversityofSciencea... 相似文献
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Magnetocaloric effect and magnetic properties of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4 and its hydride La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 were investigated. The Curie temperature of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4 was increased by hydrogen absorption. XRD patterns showed that the structure of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 remained NaZn13-type. The Curie temperature (TC) of the sample was increased from 174 K to 331 K. The homogeneity of the hydrogen absorption for La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 was proven very well by the random measurement of DSC. The magnetic entropy △SM of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4H1.6 had peak at 326 K. The peak value of-△SM-was 12.3 and 7.8 J/(kg.K) under magnetic field change of 0-2 T and 0-1 T,respectively,which was comparable with Gd5Si2Ge2. The negative slope and inflection point of the Arrott curve indicated that the first-order magnetic transition of La0.9Ce0.1(Fe0.99Mn0.01)11.6Si1.4 was reserved after hydrogen absorption. 相似文献