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1.
钢大气腐蚀锈层的红外、拉曼光谱研究   总被引:3,自引:0,他引:3  
运用红外光谱、拉曼光谱分析的方法,对碳钢A3和低合金钢10CrMoAl经青岛大气腐蚀的锈层样品,进行了比较测试,综合分析得出锈层中主要组成物相为α-Fe2O3,γ-FeOOH, α-FeOOH, δ-FeOOH,Fe3O4,以及各组成物相相对含量随腐蚀时间的变化情况。  相似文献   

2.
钢大气腐蚀锈层的激光拉曼光谱研究   总被引:1,自引:0,他引:1  
杨晓梅 《光散射学报》2007,19(2):134-137
本文运用激光拉曼光谱分析方法,对碳钢A3、低合金钢10CrMoAl经青岛大气腐蚀的锈层样品进行了比较测试,由实验结果分析得出锈层主要组成物相为α-Fe2O3,γ-FeOOH,α-FeOOH,δ-FeOOH,激光拉曼光谱分析为大气腐蚀锈层物相的研究提供有力的实验依据。  相似文献   

3.
Nd-Fe-B永磁合金腐蚀产物的拉曼光谱研究   总被引:1,自引:0,他引:1  
本文应用拉曼光谱法,研究了Nd—Fe—B永磁合金在NaCl,NaHSO_4水溶液及大气环境中的腐蚀产物组成及其变化。测定结果表明,Nd—Fe—B合金大气腐蚀产物的主要组成为:Nd(OH)_3,γ—FeOOH,α—FeOOH,Fe_3O_4及B_2O_3,在NaCl溶液中则有NdCl_3生成。在不同PH值的NaHSO_4溶液中,锈层的组成有所变化。据此,对Nd—Fe—B合金的腐蚀过程与机理进行了探讨。  相似文献   

4.
P110钢CO2腐蚀产物膜的XPS分析   总被引:6,自引:0,他引:6  
为了确定CO2腐蚀产物膜的组成及不同层次结构中成分和含量的差异,采用P110钢在高温高压腐蚀静态釜中制备CO2腐蚀产物膜,利用SEM观察了腐蚀产物膜的表面和断面形貌,结合XRD分析结果,通过XPS研究了两层结构膜的化学组成差异。结果表明,腐蚀产物膜断面呈现双层结构;膜层的主要成分是FeCO3,还有少量的CaCO3和铁的氧化物,但内层CaCO3较多且夹杂着Fe3C和单质Fe,外层氧化物稍多;通过内外层Ca^2+含量差异推断出内层腐蚀膜优先形成。  相似文献   

5.
利用脉冲激光诱导击穿光谱仪(LIBS)结合SEM、EDX和维氏硬度(HV)等分析手段,分析了316L不锈钢在350℃的液态锂中静态腐蚀500h后的腐蚀特性.微观形貌分析表明:样品存在较明显的晶间腐蚀,其腐蚀层厚度约为2.7μm.硬度分析表明:腐蚀后表面硬度值约HV234.72,约是腐蚀前硬度值的0.78倍.LIBS组分分析表明:经液态锂腐蚀后的样品表面Ni、Cr等元素含量相对减少;在被腐蚀区域Li元素含量随激光击打深度的增加而减少,而Ni、Cr等元素含量与之近似呈成正比递增;母材区Li元素的渗透深度约3.5μm,约是焊缝区的0.6倍.  相似文献   

6.
利用脉冲激光诱导击穿光谱仪(LIBS)结合SEM、EDX和维氏硬度(HV)等分析手段,分析了316L不锈钢在350℃的液态锂中静态腐蚀500h后的腐蚀特性。微观形貌分析表明:样品存在较明显的晶间腐蚀,其腐蚀层厚度约为2.7μm。硬度分析表明:腐蚀后表面硬度值约HV234.72,约是腐蚀前硬度值的0.78倍。LIBS组分分析表明:经液态锂腐蚀后的样品表面Ni、Cr等元素含量相对减少;在被腐蚀区域Li元素含量随激光击打深度的增加而减少,而Ni、Cr等元素含量与之近似呈成正比递增;母材区Li元素的渗透深度约3.5μm,约是焊缝区的0.6倍。  相似文献   

7.
本文报道了用钽片蒸发器微量取样感耦等离子体发射光谱(ICP-AES)方法,结合阳极氧化和化学腐蚀剥层技术,测定厚度1—3微米的化合物半导体外延层材料Ga_(1-x)Al_xAs中Ga和Al的原子比及其深度分布。单层或多层结构的Ga_(1-x)Al_xAs/GaAs外延层材料先经恒流阳极氧化,再用20微升盐酸腐蚀液溶解生成的氧化膜,然后用微量取样ICP-AES方法同时分析溶解液中Ga和Al的含量,并求出两者的原子比。连续多次进行阳极氧化、化学腐蚀剥层,可以测定原子比值的深度分布。二十次测定x值的相对标准偏差为2—3%。本文的结果表明,微量取样ICP-AES分析方法可以应用于各种多元化合物半导体材料中组分元素原子比的测定,并且操作简便,分析精度较高。  相似文献   

8.
氧化镁薄膜的腐蚀速率研究   总被引:1,自引:0,他引:1  
蔡长龙  刘欢  马卫红  刘卫国 《光子学报》2006,35(10):1547-1550
研究了以氧化镁(MgO)为牺牲层材料制作热成像阵列器件过程中MgO膜层在磷酸溶液中的湿法腐蚀特性,包括横向腐蚀速率和纵向腐蚀速率,获得了MgO膜层的腐蚀速率随磷酸溶液浓度和温度变化的关系曲线,并得到了用于制作图形和制作悬空结构的较好工艺参量.  相似文献   

9.
采用背散射电子扫描显微镜、电子衍射能谱和X射线衍射等分析方法,研究了浸泡在300~700℃的液态锡(Sn)中24h后的低活化马氏体/铁素体钢CLF-1的腐蚀行为。研究结果表明,在所有测试温度下液态锡对CLF-1钢表面均有不同程度的腐蚀,主要腐蚀机制为化合溶解腐蚀。铬(Cr)以单质形式溶解沉淀,液态锡与铁在CLF-1钢表面反应生成由铁锡化合物构成的腐蚀层。当温度低于500℃时,腐蚀层厚度近似为一常量,约8μm,化学成分为FeSn2。当温度高于500℃时,腐蚀层厚度随温度线性增加,腐蚀层呈双层结构,分别为CLF-1边界处的FeSn层和覆盖在其表面的FeSn2层。  相似文献   

10.
采用不同脉冲能量激光对Inconel X-750镍基合金试样进行激光喷丸(LP)强化处理,研究了不同条件下试样的热腐蚀行为,阐述了激光喷丸改善抗热腐蚀性能的机理。结果表明,LP试样的腐蚀速度明显低于未处理试样的,且激光脉冲能量越高,LP试样的腐蚀速度越低。未处理试样在热腐蚀60h后出现了两层腐蚀层,外部腐蚀层严重腐蚀并出现断裂和剥落现象。LP试样在腐蚀60h后只出现了内部氧化层,激光喷丸诱导的残余应力层有效避免了氧化膜破裂。  相似文献   

11.
Yamashita  M.  Uchida  H. 《Hyperfine Interactions》2002,139(1-4):153-166
A rust layer, so called protective rust layer, on a weathering low-alloy steel has strong protective ability for atmospheric corrosion of the steel. We have recently found through a large number of spectroscopic studies including Mössbauer spectroscopy that the protective rust layer forms after long-term phase transformation. The phase and structure of the rust definitely control the protective ability of the rust layer. From this recent knowledge, some new technologies have been developed. One is the surface-treatment technique that provides a possibility for obtaining the protective rust layer in a relatively short period even in the severe environments such as in marine and chloride (de-icing salts) containing environments. Others are based on selection of effective alloying elements for steel materials. These are particularly important for application in areas where protective rust layer formation may be hindered or prevented. In this paper, we mention recent progress in research and development on rusting protection by rust for atmospheric corrosion of steels in Japan.  相似文献   

12.
Four samples of steels with alloying elements were exposed to an industrial environment during 1,955 days, aiming to elucidate the effect of the alloying elements Cu and Ni on the resistance of weathering steels to corrosion processes. The samples were characterized with optical microscopy, scanning electron microscopy (SEM), powder X-ray diffraction (XRD), saturation magnetization measurements and with energy dispersive (EDS), infrared, Mössbauer and Raman spectroscopies. All the steels originated orange and dark corrosion layers; their thicknesses were determined from the SEM images. EDS data of such rust layers showed that the alloying element content decreases from the steel core towards the outer part of the rust layer. Moreover, in the dark rust layer some light-gray regions were identified in the W and Cu-alloy steel, where relatively higher Cr and Cu contents were found. XRD patterns, infrared, Raman and Mössbauer spectra (298, 110 and 4 K) indicated that the corrosion products are qualitatively the same, containing lepidocrocite (γFeOOH; hereinafter, it may be referred to as simply L), goethite (αFeOOH; G), feroxyhite (δ′FeOOH; F), hematite (αFe2O3; H) and magnetite (Fe3O4; M) in all samples; this composition does not depend upon the steel type, but their relative concentrations is related to the alloying element. Mössbauer data reveal the presence of (super)paramagnetic iron oxides in the corrosion products. Saturation magnetization measurements suggest that feroxyhite may be an occurring ferrimagnetic phase in the rust layer.  相似文献   

13.
The oxidation state of iron oxide nanoparticles was determined using the two principally different technical realisations of energy filtering TEM, in one case using the JEOL 3010 equipped with a LaB6 cathode and a post-column GIF and in the second, the newly designed LIBRA 200FE equipped with an corrected in-column 90 degrees energy filter and a field emission gun (Schottky emitter). The samples studied were oxide-coated iron nanoparticles, and iron oxide inclusions in feldspars in granites. Five possible candidates exist for the iron-oxide phases: FeO, alpha-Fe2O3 (hematite), gamma-Fe2O3 (maghemite), Fe3O4 (magnetite) or alpha-FeO(OH) (goethite). Fingerprinting the O K-edge ELNES allows to distinguish between oxide phases with the same stochiometry and enables to make a first selection of possible candidates. The additional determination of the chemical composition allows unique identification of the phase present. For the oxide coated iron nanoparticles the most probable iron oxide phase of the shell is maghemite, which was additionally confirmed by HRTEM studies. The second studied system were iron oxide needles in alkali feldspar, where we obtained hematite as the most probable phase. There we additionally demonstrated the drastic changes of the ELNES of the O K-edge for the alkali feldspar and iron oxide needle by spatially resolved EELS.  相似文献   

14.
张大成  马新文  朱小龙  李斌  祖凯玲 《物理学报》2008,57(10):6348-6353
激光诱导击穿光谱(LIBS)在植物样品上面的应用是一个较新的课题. 为将LIBS技术能实际应用于与食品安全相关的领域,实验中对三种真空冻干水果样品进行了初步LIBS实验研究,鉴别了其LIBS光谱,并选取典型光谱线,运用统计学方法分析比较了三种水果中Ca,Na,K,Fe,Al,Mg六种元素含量的差别. 实验结果表明,苹果中Na的含量最高,Ca的含量最低,三种水果样品中的K,Fe,Mg等元素含量也都有差异. 实验结果还表明LIBS技术是一种检测、对比植物样品中微量元素含量的有效手段. 关键词: 激光诱导击穿光谱 等离子体 植物样品 微量元素  相似文献   

15.
Qualitative and quantitative analysis of lignite coal and its ash samples taken from Soma-Darkale region in city of Manisa (Turkey) have been performed by using the EDXRF technique. Samples are prepared from powder sifted by 200 mesh sieve.The elements Fe and Ba in the samples are analysed using the standard addition method. The samples were excited by gamma rays emitted from radioisotope source. The characteristic K X-rays emitted from samples were counted by means of Si(Li) detector which has a resolution at .  相似文献   

16.
原子吸收光谱法测定膜荚黄芪不同器官矿质元素含量   总被引:1,自引:0,他引:1  
应用混合酸HNO3-HClO4 (4∶1) 在常压微沸条件下对膜荚黄芪根系及茎叶样品进行消解,采用原子吸收光谱法测定了膜荚黄芪不同器官即根及茎叶中五种人体必需矿质元素K,Fe,Zn,Mn和Cu含量,并对结果进行了统计分析与比较。该方法标准曲线相关系数为0.997 3~0.999 9, 加标回收率为92.88%~109.25%, 相对标准偏差(RSD,n=5) 为0.393 5%~3.175 2%。方法简单,结果可靠。结果显示,膜荚黄芪根及茎叶中5种矿质元素含量顺序均为K>Fe>Zn>Mn>Cu。膜荚黄芪不同器官矿质元素含量不同,根中富含Fe,Zn,Cu元素,根内Fe含量是茎叶的1.54倍。茎叶中也含有丰富的矿质元素,特别是K和Mn元素。茎叶中K含量是根的1.63倍,这与黄芪的药效相符合。试验结果将为研究矿质元素在黄芪植株中的分布以及矿质元素含量与黄芪药效相关性提供理论依据。  相似文献   

17.
We present the results of a systematic study performed by micro‐Raman spectroscopy on pure anatase, pure rutile and mixed anatase–rutile TiO2 thin films, deposited by radio frequency magnetron sputtering on quartz substrates, with different thicknesses. The crystal structures of the as‐deposited films were unambiguously determined and a good crystalline homogeneity was revealed by a systematic mapping of the samples. In the mixed‐phase films, the relative amount of the two phases was monitored by a simple analysis of the components of the multi‐Lorentzian fitting curves. For the single‐phase films, the influence of the thickness and the effect of different thermal treatments, carried out to obtain series of thin films differing only for oxygen content, are discussed. The analysis of the scattered light has provided indication about the presence of an interface layer between the substrate and the film, which can play a role in driving the interesting magnetic properties exhibited by our samples, which are of potential usefulness for spintronics application. The results obtained from other techniques are briefly reported and discussed in relation to our systematic Raman characterization. This study points out how Raman investigation can provide suggestions toward the understanding of the complex physical phenomena leading to room‐temperature ferromagnetism in TiO2 thin films. Copyright © 2009 John Wiley & Sons, Ltd.  相似文献   

18.
We analyze the polarization properties of photons which are produced in the unpolarizedb-quark decay,bsg. Using the structure function formalism we carry out a general analysis of the polarization characteristics of in terms of the standard Stokes parameters. The expressions for five independent structure functions are constructed in terms of the weak magnetic transition form factors of the verticesbs andbsg. Numerical calculations of the Stokes parameters and various differential distributions forbsg are performed for the two-Higgs doublet model (2HDM). We studied the dependences of all these characteristics to the model parameters. These results were compared with the Standard Model predictions for different top quark masses. Strong sensitivity of the Stokes parameters, which defines the linear photon polarization, to the model is demonstrated.  相似文献   

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