353 resultados para MG-GD ALLOYS


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This paper addresses the explosive consolidation of amorphous cobalt-based alloys. Using the experimental setup introduced in the present paper, specimens with high compact density, excellent magnetic properties and great wearability have been made. In comparison with permalloy and ferrite, the present specimens exhibit superior magnetic properties. Therefore, the compact is deemed as being a promising material for magnetic recording heads.

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We present numerical simulations of thermosolutal convection for directional solidification of Al-3.5 wt% Ni and Al-7 wt% Si. Numerical results predict that fragmentation of dendrite arms resulting from dissolution could be favored in Al-7 wt% Si, but not in Al-3.5 wt% Ni. Corresponding experiments are in qualitative agreement with the numerical predictions. Distinguishing the two fragmentation mechanisms, namely dissolution and remelting, is critical during experiments on earth, when fluid flow is dominant. (C) 2007 COSPAR. Published by Elsevier Ltd. All rights reserved.

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A constitutive model, based on an (n + 1)-phase mixture of the Mori-Tanaka average theory, has been developed for stress-induced martensitic transformation and reorientation in single crystalline shape memory alloys. Volume fractions of different martensite lattice correspondence variants are chosen as internal variables to describe microstructural evolution. Macroscopic Gibbs free energy for the phase transformation is derived with thermodynamics principles and the ensemble average method of micro-mechanics. The critical condition and the evolution equation are proposed for both the phase transition and reorientation. This model can also simulate interior hysteresis loops during loading/unloading by switching the critical driving forces when an opposite transition takes place.

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(Ga, Gd, As) film was fabricated by the mass-analyzed dual ion-beam epitaxy system with the energy of 1000 eV at room temperature. There was no new peak found except GaAs substrate peaks (0 0 2) and (0 0 4) by X-ray diffraction. Rocking curves were measured for symmetric (0 0 4) reflections to further yield the lattice mismatch information by employing double-crystal X-ray diffraction. The element distributions vary so much due to the ion dose difference from AES depth profiles. The sample surface morphology indicates oxidizing layer roughness is also relative to the Gd ion dose, which leads to islandlike feature appearing on the high-dose sample. One sample shows ferromagnetic behavior at room temperature. (C) 2003 Elsevier B.V. All rights reserved.

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对室温条件下用低能离子束沉积得到的 Ga As∶ Gd样品 ,借助 X射线衍射 (XRD)和高分辨 X射线衍射 (HR-XRD)进行了结构分析 ,结果表明没有出现新的衍射峰 ,并且摇摆曲线的形状与 Gd的注入计量密切相关 .运用 X光电子能谱仪对比分析了 Gd注入后 ,衬底中主要元素 Ga2 p和 As3d的化学位移 ,以及不同计量的样品中注入的Gd4 d芯能级束缚能的变化 ,并分析了铁磁性产生的可能原因 .

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室温条件下 ,用离子束外延设备制备 ( Ga,Gd,As)样品 ,X射线衍射 ( XRD)结果表明除了 Ga As衬底峰 ,没有发现其他新相的衍射峰。俄歇电子能谱 ( AES)分析了样品中元素随深度的变化 ,不同样品中元素的分布有着不同的特点。并运用原子力显微镜 ( AFM)研究了样品表面的形貌特点 ,表明样品表面的粗糙度与 Gd注入过程中在样品表面沉积的多少有关。运用交变梯度磁强计 ( AGM)对薄膜进行磁性分析 ,结果表明有的样品在室温条件下出现铁磁性 ,但金属钆本身具有室温铁磁性 ,因而需要进一步分析。

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 室温条件下,用低能离子束外延制备了GaAs∶Gd薄膜,X射线衍射(XRD)结果表明除了GaAs衬底峰没有发现其它新相的衍射峰,并借助于高分辨X射线衍射(HR XRD)进一步分析了晶格常数的变化特点。俄歇电子能谱(AES)分析了样品表面的成分,及元素随深度的分布规律,在60nm深处元素的相对含量发生明显改变,运用原子力显微镜(AFM)揭示了样品表面的形貌特点。

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Niobium-silicide alloys have great potential for high temperature turbine applications. The two-phase Nb/Nb5Si3 in situ composites exhibit a good balance in mechanical properties. Using the 52 in drop tube, the effect of undercooling and rapid solidification on the solidification process and micro-structural characterization of Nb-Si eutectic alloy was studied. The microstructures of the Nb-Si composites were investigated by optics microscope (OM), X-ray diffraction (XRD) and scanning electron microscope (SEM) equipped with X-ray energy dispersive spectrometry (EDS). Up to 480 K, deep undercooling of the Nb-Si eutectic samples was successfully obtained, which corresponds to 25% of the liquidus temperature. Contrasting to the conventional microstructure usually found in the Nb-Si eutectic alloy, the microstructure of the undercooled sample is divided into the fine and coarse regions. The most commonly observed microstructure is Nb+Nb5Si3, and the Nb3Si phase is not be found. The change of coarseness of microstructure is due to different cooling rates during and after recalescence. The large undercooling is sufficient to completely bypass the high temperature phase field.

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This study focuses on mechanism of ceramic coating on Al-Si alloys with bulk primary Si using plasma electrolytic oxidation (PEO) technology. Al-Si alloys with 27-32% Si in weight were used as substrates. The morphologies, composition and microstructure of PEO coatings were investigated by scanning electron microscopy (SEM) with energy dispersive X-ray system (EDX). Results showed that the PEO process had four different stages. The effect of bulk Si is greatly on the morphology and composition of coatings at first three stages. Anodic oxide films formed on Al and Si phases, respectively. When the voltage exceeded 40 V, glow appeared and concentrated on the localized zone of interface of Al and Si phase. Al-Si-O compounds formed and covered on the dendrite Si phase surface, and the coating on bulk Si, which was silicon oxide, was rougher than that on other phase. If the treatment time was long enough, the coatings with uniform surface morphologies and elements distribution will be obtained but the microstructure of inner layer is looser due to the bulk Si.

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Transparent polycrystalline MgO and TiO2 codoped Al2O3 ceramics were fabricated by conventional solid-state pressureless processing. The absorption, emission and excitation spectra of ( Mg, Ti : Al2O3 ceramics were measured. Owing to charge compensation of Mg2+, only UV absorption around 250nm was observed due to O2- -> Ti4+ charge transfer transitions (CT) when Ti content was low. As a result, the emission peaks of isolated Ti4+ ion located at 280-290nm and 410-420nm were observed. Besides absorption peak of V, ion, the characteristic absorption peak of V, ion centered at 490nm was observed in Mg, Ti) : Al2O3 ceramics when Ti content was high. The emission spectra of Ti3+, ion in polycrystalline Al2O3 ceramics coincide with that of Ti: Al2O3 single crystal.

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Er3+ -doped Gd2SiO5 (Er:GSO) single crystal with dimensions of circle divide 35 x 40 mm(3) has been grown by the Czochralski method. The absorption and fluorescence spectra of the Er:GSO crystal were measured at room temperature. The spectral parameters were calculated based on Judd-Ofelt theory, and the intensity parameters Omega(2), Omega(4) and Omega 6 are obtained to be 6.168 x 10(-20), 1.878 x 10(-20), and 1.255 x 10(-20) cm(2), respectively. The emission cross-section has been calculated by Fuechtbauer-Ladenbury formula. (c) 2007 Elsevier B.V. All rights reserved.

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火炬松(Pinus taeda L.)原产美国东南部,是世界南方松中最重要的绿化和造林用速生针叶树种,现广泛分布于全球亚热带和部分热带地区,在我国的栽植面积居世界第2位,仅次于美国。目前,火炬松离体快速繁殖、遗传转化和品种改良研究中最大的障碍是没有获得良好的植株再生体系。本研究以火炬松的成熟种子为试材,建立了可调控的体细胞胚胎发生和器官发生植株再生系统,并对再生过程中的形态学变化进行了细胞学观察和扫描电镜观察;建立了胚性细胞悬浮系,测定了其重要生长参数的变化动态,优化了悬浮条件下体细胞胚胎发生的培养条件及悬浮细胞原生质体直接体细胞胚胎发生的培养条件。 进行了HA、HB、HC、MA、MB、MC、LA和LB等8种不同基因型的成熟合子胚在BMS、DCR、GD、LM、LP、MNCI、MS、SH及自行设计的TE等9种不同基本培养基上的愈伤组织诱导试验,筛选获得了愈伤组织发生频率较高的基因型HB、MA和MC,及基本培养基DCR和TE。激素组合试验表明,2,4-D和BA最有利于愈伤组织发生。两因子5水平等重复的愈伤组织诱导试验及方差分析结果证实,8 mg•L~(-1)2,4-D和4 mg•L~(-1)BA是愈伤组织诱导的最佳激素组合。诱导产生的愈伤组织经2次继代后,可明显分为4种类型,它们是1)白色、半透明、有光泽的粘性愈伤组织(WTGM);2)淡黄色、疏松、有光泽的颗粒状愈伤组织(YLGG);3)淡绿色、疏松的颗粒状愈伤组织(GLG);和4)浅白色、水浸状的粘性愈伤组织(WMM)。其中白色、半透明、有光泽的粘性愈伤组织有较强的体细胞胚胎发生能力,淡黄色、疏松、有光泽的颗粒状愈伤组织有较强的不定芽发生能力。这两种愈伤组织的最高诱导频率分别是28.1%和35.7%。 在附加2,4-D、IBA和BA的DCR体细胞胚诱导培养基上,白色、半透明、有光泽的粘性愈伤组织中的胚性细胞形成胚性胚柄细胞团和早期原胚。提高培养基中的渗透压后,早期原胚发育成后期原胚。在附加ABA、PEG和活性炭的DCR体细胞胚成熟培养基上,后期原胚发育成子叶胚。在无激素DCR培养基上,子叶胚萌发形成再生完整植株。体细胞胚转换成小植株的最高频率是18.4%。在直接体细胞胚诱导增养基和直接体细胞胚发育培养基的作用下,成熟合子胚的子叶和胚轴上直接形成体细胞胚。直接体细胞胚胎发生的最高频率是18%。 在附加NAA、IBA和BA的TE不定芽原基诱导培养基上,淡黄色、疏松、有光泽的颗粒状愈伤组织中的胚性细胞形成不定芽原基。在附加IBA和BA的TE不定芽分化培养基上,不定芽原基分化产生不定芽。用基因型HB、MA和MC的淡黄色、疏松、有光泽的颗粒状愈伤组织进行的试验表明,不定芽分化的最佳低温(4 ℃)处理时间是5~6周,最佳蔗糖浓度是25~30 g•L~(-1)。分化产生的不定芽在附加IBA、GA_3和活性炭的TE培养基上,幼茎伸长。附加IBA、BA和GA_3的TE培养基上,伸长的不定芽生根形成完整植株。伸长不定芽的最高生根频率是46%。成熟合子胚在直接不定芽原基诱导培养基及直接不定芽分化培养基的作用下,从子叶和胚轴的不同部位产生直接不定芽。直接不定芽发生的最高频率是58.2%。 由成熟合子胚诱导愈伤组织形成过程中的形态学观察表明:在附加2,4-D和BA的DCR愈伤组织诱导培养基上,HB、MA和MC3种基因型中,MA主要在下胚轴形成愈伤组织,MC主要在子叶和胚根形成愈伤组织,HB主要在胚根形成体积较小的愈伤组织。在附加NAA和BA的TE愈伤组织诱导培养基上,HB、MA和MC3种基因型中,MA在单个子叶的顶端形成生长较快的愈伤组织,MC的所有子叶都形成愈伤组织,HB在所有子叶的顶端形成愈伤组织。 石蜡切片观察表明:4类愈伤组织的细胞组成不同.第1类愈伤组织主要由核大、质浓、体积小的园形胚性细胞及核呈柱状或新月形的体积较大的非胚性细胞组成;第2类愈伤组织主要由核大、质浓、体积小的园形胚性细胞组成,第3类愈伤组织主要由体积较大的棒状、葫芦形、新月形、盾片状细胞组成、第4类愈伤组织主要由体积较大的薄壁细胞和细胞壁加厚、细胞间连结紧密、无细胞核的分化细胞组成,第1类愈伤组织上形成的早期原胚的特点是:胚性头部由排列紧密、体积小的园形细胞组成,轮廓十分清晰、呈半圆形,胚柄由排列疏松的长形细胞组成,细胞体积大、细胞中有大的液泡,早期原胚在发育过程中和母体组织保持一定的隔离状态。第2类愈伤组织上形成的不定芽的特点是t结构上为单极性,其维管束和母体组织保持密切联系。扫描电镜观察表明;直接体细胞胚基部和母体组织保持较少的联系,其子叶是直立生长的.直接不定芽基部和母体组织保持较多的联系,其幼叶是向心卷曲生长的。 在培养周期内,基因型HB、MA和MC胚性细胞悬浮培养物的几个生长参数的变化动态相似。鲜重增长高峰在12—15 d,干重增长高峰在15~18 d,细胞体积增长高峰和胚数增长高峰在18—21 d。在培养的18—21 d,培养液中的pH值、电导率和蔗糖浓度接近或降到最低点。在悬浮培养条件下,体细胞胚形成的最佳起始细胞密度是5~6×103个/ml。继代培养时间延长,体细胞胚胎发生能力下降。热激处理促进基因型HB和MA体细胞胚的形成,抑制基因型MC体细胞胚的形成。在悬浮培养物中,观察到了裂生多胚。 对数生长期的火炬松胚性悬浮细胞,在以甘露醇作为渗透压稳定剂的酶混合液Cel-lulase“Onozuka”RS l%+Cellulase“Onozuka”R-10 2.5%+Pectolyase Y-23 0.2%的作用下,原生质体的产量和活力均最高。原生质体在DCR和KM8P两种培养基上形成了体细胞胚(包括胚性胚柄细胞团、早期原胚和后期原胚).体细胞胚形成的最佳起始原生质体密度是7×l04个/ml,最佳ABA浓度是4 mg.L-I.