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《2024年近红外给体-受体AIE分子设计合成及光诊疗研究》范文

《2024年近红外给体-受体AIE分子设计合成及光诊疗研究》范文

《近红外给体-受体AIE分子设计合成及光诊疗研究》篇一近红外给体-受体E分子设计合成及光诊疗研究一、引言随着科技的飞速发展,光诊疗技术已成为现代医学领域的重要研究方向。

其中,近红外给体-受体E(聚集诱导发光)分子因其独特的发光性能和生物相容性,在生物成像、光动力治疗等领域展现出巨大的应用潜力。

本文旨在探讨近红外给体-受体E分子的设计合成方法,以及其在光诊疗领域的应用研究。

二、近红外给体-受体E分子的设计原理近红外给体-受体E分子的设计主要基于分子内电荷转移(ICT)理论和聚集诱导发光(E)效应。

设计过程中,需考虑分子的给体和受体部分、分子结构中的共轭体系、以及分子内的电子云分布等因素。

近红外区域的光子能量较低,能够深入组织内部,具有较低的背景噪声和较高的组织穿透力,因此,设计合成近红外发光的E分子具有重要意义。

三、分子合成方法近红外给体-受体E分子的合成主要采用有机合成方法。

首先,根据设计原理,选择合适的给体和受体部分,通过化学反应将它们连接起来。

在合成过程中,需要严格控制反应条件,如温度、时间、溶剂等,以保证分子结构的稳定性和纯度。

此外,还需对合成得到的分子进行表征,如核磁共振、紫外-可见吸收光谱、荧光光谱等,以验证其结构和性能。

四、光诊疗应用研究1. 生物成像近红外给体-受体E分子在生物成像领域具有广泛的应用。

由于其发光强度高、背景噪声低、组织穿透力强等特点,使得其在细胞成像、组织成像等方面具有显著优势。

通过将E分子与生物分子或细胞标记物结合,可以实现高分辨率、高灵敏度的生物成像。

2. 光动力治疗光动力治疗是一种利用光敏剂和光照治疗肿瘤的方法。

近红外给体-受体E分子可作为光敏剂,在光照下产生单线态氧等活性氧物质,对肿瘤细胞产生杀伤作用。

此外,E分子的近红外发光性能有助于实时监测光动力治疗过程,为临床治疗提供有力支持。

五、实验结果与讨论通过合成不同结构的近红外给体-受体E分子,并对其在生物成像和光动力治疗中的应用进行研究。

清华大学多层石墨烯电子皮肤可靠贴合监测人体信号

清华大学多层石墨烯电子皮肤可靠贴合监测人体信号
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噬菌体展示技术筛选脑靶向功能肽及其修饰纳米粒的脑内递药研究

噬菌体展示技术筛选脑靶向功能肽及其修饰纳米粒的脑内递药研究

噬菌体展示技术筛选脑靶向功能肽及其修饰纳米粒的脑内递药研究一、概述在生物医学领域中,脑靶向递药系统一直是研究的热点和难点。

由于血脑屏障的存在,许多药物难以有效进入大脑,从而限制了其在中枢神经系统疾病治疗中的应用。

开发新型的脑靶向递药技术,对于提高药物在脑部的浓度和疗效,降低副作用具有重要意义。

噬菌体展示技术以其独特的优势在药物研发和生物医学领域得到广泛应用。

该技术通过将外源蛋白或多肽的DNA序列插入到噬菌体外壳蛋白结构基因的适当位置,使外源基因随外壳蛋白的表达而表达,同时外源蛋白随噬菌体的重新组装而展示到噬菌体表面。

利用噬菌体展示技术,我们可以筛选到与特定靶标具有高亲和力的多肽或蛋白,为药物研发和疾病治疗提供新的候选分子。

本研究旨在利用噬菌体展示技术筛选具有脑靶向功能的多肽,并将其修饰到纳米粒表面,构建新型的脑靶向递药系统。

通过优化筛选条件和方式,我们成功获得了多个具有脑靶向功能的多肽序列,并通过实验验证了其脑靶向性。

我们还将这些多肽以共价连接的方式修饰到聚乙二醇聚乳酸羟基乙酸共聚物(PEGPLGA)纳米粒表面,以提高药物的稳定性和脑部递送效率。

本研究不仅为脑靶向递药系统的开发提供了新的思路和方法,还为中枢神经系统疾病的治疗提供了新的候选药物和递送策略。

通过进一步的研究和优化,我们相信这种新型的脑靶向递药系统将在未来为更多的患者带来福音。

1. 介绍脑靶向药物递送的重要性与挑战脑靶向药物递送是神经科学领域的一个关键研究方向,对于治疗脑部疾病具有重要意义。

由于血脑屏障的存在,许多药物难以有效穿透并进入脑组织,这使得脑内疾病的治疗面临着巨大的挑战。

开发高效的脑靶向药物递送系统成为当前研究的热点和难点。

脑靶向药物递送的重要性主要体现在以下几个方面:对于脑部疾病如阿尔茨海默病、帕金森病、脑肿瘤等,有效的药物递送能够显著提高治疗效果,改善患者的生存质量。

脑靶向递送系统能够实现药物的精准定位,减少对其他组织器官的副作用。

WC-Co硬质合金制备中铝元素对钨产品的影响

WC-Co硬质合金制备中铝元素对钨产品的影响

WC-Co硬质合金制备中铝元素对钨产品的影响朱红波;杨欣;谭敦强;李亚蕾;何文;汤斌兵【摘要】在仲钨酸铵(ammonium paratungstate,APT)中添加一定量的Al(NO3)3·9H2O,制得Al含量(质量分数)为1.0%的APT-Al复合粉末.经煅烧、还原、碳化和液相烧结,分别得到含Al的W粉、WC粉及WC-Co硬质合金等钨产品.通过X线衍射(XRD)、场发射扫描电镜(FESEM)和高分辨透射电镜(HRTEM)对W及WC粉的形貌及结构进行分析,并分析Al元素在几种钨产品中的分布,研究WC-Co硬质合金制备过程中Al元素的相演变情况,以及Al元素对各阶段钨产品组织形貌与结构的影响.结果表明:在WC-Co硬质合金的制备过程中,Al元素经历Al2(WO4)3—AlWO4—Al4C3的相演变.Al2(WO4)3和AlWO4阻碍W颗粒通过"挥发-沉积"机制而长大,导致钨粉细化;Al4C3颗粒分布于WC颗粒之间,并阻碍细小WC颗粒通过晶界迁移而长大;WC-Co硬质合金中的Al元素主要分布在Co粘结相中以及细小WC颗粒聚集处,使得合金的致密度、硬度和断裂韧性都降低.【期刊名称】《粉末冶金材料科学与工程》【年(卷),期】2016(021)002【总页数】7页(P202-208)【关键词】Al元素;钨;碳化钨;WC-Co硬质合金;相演变【作者】朱红波;杨欣;谭敦强;李亚蕾;何文;汤斌兵【作者单位】南昌大学材料科学与工程学院,南昌 330031;南昌大学材料科学与工程学院,南昌 330031;南昌大学材料科学与工程学院,南昌 330031;南昌大学材料科学与工程学院,南昌 330031;南昌大学材料科学与工程学院,南昌 330031;南昌大学材料科学与工程学院,南昌 330031【正文语种】中文【中图分类】TF125钨因具有高熔点、高强度、高硬度、高导热性能及低溅射率等性质,广泛应用于硬质合金、钨基高密度合金、钨丝、钨电极等众多领域[1−6]。

定量电子显微学方法与氧化钛纳米结构研究获国家自然科学二等奖

定量电子显微学方法与氧化钛纳米结构研究获国家自然科学二等奖
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新型光学活性含氰基三联苯液晶聚噻吩合成与分子构象(英文)

新型光学活性含氰基三联苯液晶聚噻吩合成与分子构象(英文)
质进行 了表征. 单体都呈现 出良好的液晶性 能, 由于长间隔基 的存 在, 聚合物 P () P C T 6T h N也 呈现出 良好 S d mA
相. 氰基三联苯 的存在还赋予 了聚合物 良好 的光致发光性 能, 同时, 长间隔基也有效地降低 了分 子间的相互作
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半导体量子点内弹性应变能的研究(英文)

半导体量子点内弹性应变能的研究(英文)

半导体量子点内弹性应变能的研究(英文)
杨红波;俞重远;刘玉敏;黄永箴
【期刊名称】《人工晶体学报》
【年(卷),期】2004(33)4
【摘要】本文用有限元分析软件ANSTS 6 .0计算了半导体量子点内的弹性应变和弹性应变能 ,通过对金塔形、台形和圆顶形量子点内总弹性应变能的计算和总能量的比较 ,得到了在热平衡条件下金字塔形量子点是最稳定的结构。

【总页数】4页(P531-534)
【关键词】有限元分析软件;半导体量子点;弹性应变;弹性应变能
【作者】杨红波;俞重远;刘玉敏;黄永箴
【作者单位】北京邮电大学理学院;中国科学院半导体研究所,集成光电子学国家重点联合实验室
【正文语种】中文
【中图分类】O472
【相关文献】
1.异质外延自组织量子点弹性应变场分布的研究 [J], 刘玉敏;俞重远;杨红波;黄永箴
2.剩余应变对半导体量子点边带能影响的数值分析 [J], 杨红波;俞重远
3.Ge/Si半导体量子点的应变分布与平衡形态 [J], 蔡承宇;周旺民
4.有限元法分析透镜形自组织生长量子点的弹性应变场分布(英文) [J], 刘玉敏;俞
重远;杨红波;黄永箴
5.1.55μm张应变InGaAsP/InGaAsP量子阱偏振不灵敏半导体光放大器的优化设计(英文) [J], 邱伟彬;何国敏;董杰;王圩
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基于自转一阶非连续式微球双平盘研磨的运动学分析与实验研究

基于自转一阶非连续式微球双平盘研磨的运动学分析与实验研究

第53卷第8期表面技术2024年4月SURFACE TECHNOLOGY·133·基于自转一阶非连续式微球双平盘研磨的运动学分析与实验研究吕迅1,2*,李媛媛1,欧阳洋1,焦荣辉1,王君1,杨雨泽1(1.浙江工业大学 机械工程学院,杭州 310023;2.新昌浙江工业大学科学技术研究院,浙江 绍兴 312500)摘要:目的分析不同研磨压力、下研磨盘转速、保持架偏心距和固着磨料粒度对微球精度的影响,确定自转一阶非连续式双平面研磨方式在加工GCr15轴承钢球时的最优研磨参数,提高微球的形状精度和表面质量。

方法首先对自转一阶非连续式双平盘研磨方式微球进行运动学分析,引入滑动比衡量微球在不同摩擦因数区域的运动状态,建立自转一阶非连续式双平盘研磨方式下的微球轨迹仿真模型,利用MATLAB对研磨轨迹进行仿真,分析滑动比对研磨轨迹包络情况的影响。

搭建自转一阶非连续式微球双平面研磨方式的实验平台,采用单因素实验分析主要研磨参数对微球精度的影响,得到考虑圆度和表面粗糙度的最优参数组合。

结果实验结果表明,在研磨压力为0.10 N、下研磨盘转速为20 r/min、保持架偏心距为90 mm、固着磨料粒度为3000目时,微球圆度由研磨前的1.14 μm下降至0.25 μm,表面粗糙度由0.129 1 μm下降至0.029 0 μm。

结论在自转一阶非连续式微球双平盘研磨方式下,微球自转轴方位角发生突变,使研磨轨迹全覆盖在球坯表面。

随着研磨压力、下研磨盘转速、保持架偏心距的增大,微球圆度和表面粗糙度呈现先降低后升高的趋势。

随着研磨压力与下研磨盘转速的增大,材料去除速率不断增大,随着保持架偏心距的增大,材料去除速率降低。

随着固着磨料粒度的减小,微球的圆度和表面粗糙度降低,材料去除速率降低。

关键词:自转一阶非连续;双平盘研磨;微球;运动学分析;研磨轨迹;研磨参数中图分类号:TG356.28 文献标志码:A 文章编号:1001-3660(2024)08-0133-12DOI:10.16490/ki.issn.1001-3660.2024.08.012Kinematic Analysis and Experimental Study of Microsphere Double-plane Lapping Based on Rotation Function First-order DiscontinuityLYU Xun1,2*, LI Yuanyuan1, OU Yangyang1, JIAO Ronghui1, WANG Jun1, YANG Yuze1(1. College of Mechanical Engineering, Zhejiang University of Technology, Hangzhou 310023, China;2. Xinchang Research Institute of Zhejiang University of Technology, Zhejiang Shaoxing 312500, China)ABSTRACT: Microspheres are critical components of precision machinery such as miniature bearings and lead screws. Their surface quality, roundness, and batch consistency have a crucial impact on the quality and lifespan of mechanical parts. Due to收稿日期:2023-07-28;修订日期:2023-09-26Received:2023-07-28;Revised:2023-09-26基金项目:国家自然科学基金(51975531)Fund:National Natural Science Foundation of China (51975531)引文格式:吕迅, 李媛媛, 欧阳洋, 等. 基于自转一阶非连续式微球双平盘研磨的运动学分析与实验研究[J]. 表面技术, 2024, 53(8): 133-144.LYU Xun, LI Yuanyuan, OU Yangyang, et al. Kinematic Analysis and Experimental Study of Microsphere Double-plane Lapping Based on Rotation Function First-order Discontinuity[J]. Surface Technology, 2024, 53(8): 133-144.*通信作者(Corresponding author)·134·表面技术 2024年4月their small size and light weight, existing ball processing methods are used to achieve high-precision machining of microspheres. Traditional concentric spherical lapping methods, with three sets of circular ring trajectories, result in poor lapping accuracy. To achieve efficient and high-precision processing of microspheres, the work aims to propose a method based on the first-order discontinuity of rotation for double-plane lapping of microspheres. Firstly, the principle of the first-order discontinuity of rotation for double-plane lapping of microspheres was analyzed, and it was found that the movement of the microsphere changed when it was in different regions of the upper variable friction plate, resulting in a sudden change in the microsphere's rotational axis azimuth and expanding the lapping trajectory. Next, the movement of the microsphere in the first-order discontinuity of rotation for double-plane lapping method was analyzed, and the sliding ratio was introduced to measure the motion state of the microsphere in different friction coefficient regions. It was observed that the sliding ratio of the microsphere varied in different friction coefficient regions. As a result, when the microsphere passed through the transition area between the large and small friction regions of the upper variable friction plate, the sliding ratio changed, causing a sudden change in the microsphere's rotational axis azimuth and expanding the lapping trajectory. The lapping trajectory under different sliding ratios was simulated by MATLAB, and the results showed that with the increase in simulation time, the first-order discontinuity of rotation for double-plane lapping method could achieve full coverage of the microsphere's lapping trajectory, making it more suitable for precision machining of microspheres. Finally, based on the above research, an experimental platform for the first-order discontinuity of rotation for double-plane lapping of microsphere was constructed. With 1 mm diameter bearing steel balls as the processing object, single-factor experiments were conducted to study the effects of lapping pressure, lower plate speed, eccentricity of the holding frame, and grit size of fixed abrasives on microsphere roundness, surface roughness, and material removal rate. The experimental results showed that under the first-order discontinuity of rotation for double-plane lapping, the microsphere's rotational axis azimuth underwent a sudden change, leading to full coverage of the lapping trajectory on the microsphere's surface. Under the lapping pressure of 0.10 N, the lower plate speed of 20 r/min, the eccentricity of the holder of 90 mm, and the grit size of fixed abrasives of 3000 meshes, the roundness of the microsphere decreased from 1.14 μm before lapping to 0.25 μm, and the surface roughness decreased from 0.129 1 μm to 0.029 0 μm. As the lapping pressure and lower plate speed increased, the microsphere roundness and surface roughness were firstly improved and then deteriorated, while the material removal rate continuously increased. As the eccentricity of the holding frame increased, the roundness was firstly improved and then deteriorated, while the material removal rate decreased. As the grit size of fixed abrasives decreased, the microsphere's roundness and surface roughness were improved, and the material removal rate decreased. Through the experiments, the optimal parameter combination considering roundness and surface roughness is obtained: lapping pressure of 0.10 N/ball, lower plate speed of 20 r/min, eccentricity of the holder of 90 mm, and grit size of fixed abrasives of 3000 meshes.KEY WORDS: rotation function first-order discontinuity; double-plane lapping; microsphere; kinematic analysis; lapping trajectory; lapping parameters随着机械产品朝着轻量化、微型化的方向发展,微型电机、仪器仪表等多种工业产品对微型轴承的需求大量增加。

密度泛函理论

密度泛函理论
1 电荷密度拟合措施

库仑势即可按下式展开
2 电荷密度多极展开措施 (1)
将(1)式和
1 r r'
旳Laplace展开式代入,化简得
总库仑势为
七、近代密度泛函旳显体现式
1 局域密度近似LDA
将密度泛函理论旳K-S措施用于实际计算,必须懂得 或
与 旳泛函关系。这是密度泛函理论旳关键问题,对于一般体
1978年Peukert首先得到含时K-S方程,1984年Runge和Gross 基于含时薛定谔方程,严格导出含时密度泛函理论(TD-DFT)
含时K-S方程
近来单旳近似是绝热局域密度近似(ALDA或TDLDA)
含时密度泛函,都要要求懂得不处于基态时旳互换-有关问题,所以 诸多人致力于致力于这方面旳研究,其中TD-DFT响应理论比较广泛 ,其对低激发态具有很好旳计算构造,误差在0.1-1.0eV。但对高激 发态误差比较大。所以还需进一步旳工作。
无相互作用动能
则 即得Kohn-Sham方程
式中
有效势 称为互换有关势
五、某些化学概念旳明拟定义
1 电负性 1934年Mulliken根据下列推理定义电负性 设有B和D两原子,原子旳第一电离势为I 第一电子亲和能为A
这只是根据某些试验成果归纳出来旳,没有严格定量旳理论论证。
1978年Parr等从密度泛函理论出发定义电负性 (1)
根据K-S措施,设自旋轨道函数基组 {i , , } 满足条件
其中
SDFT.
相对论性密度泛函理论
在重元素原子核紧邻区域电子运动速度不高,相对论效应很明显 。化学变化是与价电子相联络旳,价电子旳运动速度并不高,因 此相对论量子力学旳奠基人Dirac以为在考虑原子和分子旳构造以及 一般化学反应时相对论效应并不主要,这一观点被普遍接受长达四 十年。在20世纪70年代前后,人们发觉这一认识具有片面性,相对 论效应对重元素化合物旳性质具有明显影响。

ct方法及配方有意义

ct方法及配方有意义

*Highlights
The highlights of the present work is as follows
The aim of this study was to investigate the physical, chemical and biological properties of the bioglass reinforced yttria-stabilized composite layer on Ti6Al4V titanium substrate for dental implant applications. Electrophoretic deposition, a simple and fast low temperature coating technique was used to prepare a bilayer coatings of YSZ (first) and Bioglass zirconia reinforced composite (second) on Ti6Al4V substrates. Biocompatible yttria-stabilized zirconia (YSZ) in the form of nano-particles and sol gel derived bioglass in the form of micro-particles were chosen as precursor materials for coatings. The first deposited layer consisted of ≈ 4-5 μm of YSZ, aiming at avoiding metal ion leach out from the substrate. The second layer consisted of ≈15 μm thick zirconia-bioglass composite, thought to react with the surrounding bone tissue and to enhance bone formation and implant fixation. The coatings were vacuum sintered at 900ºC for 3 h. The biocompatibility of the developed composite coatings were studied in osteoblast cell culture and their corrosion resistance in simulated body fluid (SBF) was exa It is suggested that Ti6Al4V implants could achieve better osseointegration, mechanical property and corrosion resistance under load-bearing conditions by depositing a zirconia and bioglass zirconia reinforced composite bilayer onto the Ti6Al4V metal substrates

国外期刊英文论文

国外期刊英文论文

Influence of Deformation
Li CL, Chen Mater. Sci. & 2002, 325: SCI a
14 Temperature on Shape Memory
DJ, Jin ZH Eng. A
375-379
EI
Effect of Fe-Mn-Si-Cr-Ni Alloy
Wang TJ
Comparison between fatigue
Qiao GJ,
Int. J. Fatigue 2002, 24(5): SCI a
17
behavior of some ceramics: a new concept of intrinsic stress-corrosion
Wang HJ, Jin ZH
Ding HF, Jin
258-264
EI
ZH
The interfacial stability of the
Tang WM,
Mater. Chem. 2002, 77:
SCI a
21 coated-SiC/Fe couple
Zheng ZX,
Phys.
Ding HF, Jin
236-241
EI
ZH
31
Unlubricated wear of Si/SiC and its composite with nickel Si/SiC-Ni
Sang KZ, Jin ZH
Tribology Int.
2001, 34(5): SCI a
315 -319
EI
Effects of crystalline morphology Xu T, Yu J, Jin Mater.

梯度纳米贝氏体化涂层剪切带增强增韧调控及其摩擦学行为研究

梯度纳米贝氏体化涂层剪切带增强增韧调控及其摩擦学行为研究

梯度纳米贝氏体化涂层剪切带增强增韧调控及其摩擦学行为研究下载提示:该文档是本店铺精心编制而成的,希望大家下载后,能够帮助大家解决实际问题。

文档下载后可定制修改,请根据实际需要进行调整和使用,谢谢!本店铺为大家提供各种类型的实用资料,如教育随笔、日记赏析、句子摘抄、古诗大全、经典美文、话题作文、工作总结、词语解析、文案摘录、其他资料等等,想了解不同资料格式和写法,敬请关注!Download tips: This document is carefully compiled by this editor. I hope that after you download it, it can help you solve practical problems. The document can be customized and modified after downloading, please adjust and use it according to actual needs, thank you! In addition, this shop provides you with various types of practical materials, such as educational essays, diary appreciation, sentence excerpts, ancient poems, classic articles, topic composition, work summary, word parsing, copy excerpts, other materials and so on, want to know different data formats and writing methods, please pay attention!摘要:本研究通过对梯度纳米贝氏体化涂层的剪切带增强增韧调控及其摩擦学行为进行深入研究,旨在探索新型涂层在材料科学与工程领域的应用潜力。

ROS响应性纳米清除剂在骨关节炎防治中的抗氧化能力和免疫调节作用

ROS响应性纳米清除剂在骨关节炎防治中的抗氧化能力和免疫调节作用

ROS响应性纳米清除剂在骨关节炎防治中的抗氧化能力和免疫调节作用1.1国内外研究现状:骨关节炎是一种以软骨细胞功能失调和炎症反应为主要特征的退行性疾病。

其发病率随着老龄化进程的加剧而持续增长。

骨关节炎的发生发展与活性氧(reactive oxygen species, ROS)的异常累积密切相关。

在骨关节炎患者的患处,ROS的表达水平明显升高,这导致软骨细胞和滑膜组织的损伤。

因此,如何有效清除和抑制ROS的生成,是当前骨关节炎研究的关键目标之一。

利用ROS响应性纳米材料设计智能的抗氧化和抗炎药物输送系统,可以实现对病灶部位ROS的高效清除和炎症抑制,从而达到精准治疗骨关节炎的目的。

这一领域国内外研究人员进行了大量探索,取得了一些进展。

国外方面,Xu等人利用多模态成像引导精确抗癌和抗炎的刺激响应纳米治疗。

该纳米粒子可以响应软骨细胞产生的ROS被降解,从而按需释放青蒿素抑制ROS生成和氧化应激。

另有研究者构建了富集一氧化碳的红细胞膜包覆纳米颗粒,一氧化碳是一种抗炎气体分子。

这种纳米颗粒可以穿透滑膜细胞层,释放一氧化碳抑制M1型巨噬细胞的激活,减轻炎症反应。

这两项研究都初步证明了ROS响应性纳米清除剂在骨关节炎治疗中的潜在价值。

除药物输送系统外,也有学者开发ROS响应性水凝胶系统治疗骨关节炎。

如等设计了富硫氢凝胶,其可在ROS环境下产生氢气充填骨关节腔,从而帮助修复软骨。

除药物输送系统外,也有学者开发ROS响应性水凝胶用于骨科疾病治疗。

国内方面, 随着中国人口的老龄化,骨关节炎的患病人数正在快速增加。

骨关节炎的发生与滑膜炎症和软骨细胞功能失调密切相关,而ROS的异常累积被认为是导致这些病理变化的重要因素之一。

因此,开发可以响应ROS并释放治疗药物的智能输送系统,实现对骨关节炎病灶的高效、精准治疗,是当前国内外研究的热点方向。

国内学者在这一领域也进行了大量探索,并取得了一些重要进展。

例如, 浙江大学的研究组合成了硫醚键交联的注射型水凝胶,可用作骨关节造影剂。

文献汇报ppt模板

文献汇报ppt模板
一.Conclusion
Xiaofang Cao, Chunying Rong, Aiguo Zhong, Tia Lu , and Shubin Liu
参考文献 Cao X, Rong C, Zhong A, et al. Molecular acidity: An accurate description with information‐theoretic approach in density functional reactivity theory[J]. Journal of Computational Chemistry, 2017. Donghai Yu, Ruobing Du,Ji-Chang Xiao,et al. Theoretical Study of pKa Values for Trivalent Rare-Earth Metal Cations in Aqueous Solution [J].Journal of Phusical Chemistry,2017
Xiaofang Cao, Chunying Rong, Aiguo Zhong, Tia Lu , and Shubin Liu
Theoretical framework
Molecular Acidity: An Accurate Description with InformationTheoretic Approach in Density Functional Reactivity Theory
4.Results and discussion
Molecular Acidity: An Accurate Description with InformationTheoretic Approach in Density Functional Reactivity Theory

边缘化学修饰锯齿型石墨烯纳米带的电子结构

边缘化学修饰锯齿型石墨烯纳米带的电子结构

1 理 论 方 法
于第一 原理 密 度 泛 函进 行模 拟 计 算 的 软 件 。结 构 优 化 过 程 中 , 用局域 密度 近似 ( D , 采 L A) 以确 定 能量 最 低 的几 何 构 型 。 在此 基础上 , 采用 广义 梯度 近似 ( G 方 法 处 理 电子 之 间相 G A)
对有限宽 Z N s其表现为半导体性 , G R, 具有 自 旋极化基态 , G R 两边局域电子态的 自 在 NS 旋方向相反。 最近 ,o 等人 报道 了外 加垂直 Z N s Sn4 G R 轴线 的 电场可使 体 系变为半 金属 态 , 即一个 自旋方 向表现 金属
性, 另一个 自旋 方 向能 隙增 大 , 相应结 果为 实验上 制备 出石 墨烯 基 自旋 开 关提 供 了重 要 的理 论 依据 。Y u等
2 2 能带结构 .
在 这部分 内容 中 , 主要 是针 对不 同边 缘饱 和 Z N s的能 带结 构进 行讨论 。 由于体 系 的 电学 性 质 主要取 GR 决 于其 费米 面附 近 的电子 结构 , 因此 , 们我 们 主要研 究 费米 面 附 近能量 在 一04 a一 .H 我 .H 0 4 a能 量 区 间的 电
其 中 -o =一70 85 aE =一 0 .2 H , E ‰ 6 .9 H 、 6 69 13 a
氧 原子 饱和 纳米 带 的结合 能
E 0= E f 一2×E 一E一 =一 5 . 5 0 6 7 9 6 4一(一2× 4 9 2— 0 . 2 )= 一1 1 1 a 7 .6 69 13 .9 H ,
过对纳米带边缘修饰来控制纳米带的电子结构 , 相应的计算结果为实验上制备石墨烯纳米带提供 了理论依
据。
参考文献 :

SYNTHESIS OF A FUNCTIONALLY GRADED PAD FOR CHEMIC

SYNTHESIS OF A FUNCTIONALLY GRADED PAD FOR CHEMIC

专利名称:SYNTHESIS OF A FUNCTIONALLY GRADED PAD FOR CHEMICAL MECHANICALPLANARIZATION发明人:MISRA, Sudhanshu,ROY, Pradip, K.,DEOPURA, Manish申请号:US2004017638申请日:20040603公开号:WO05/000529P1公开日:20050106专利内容由知识产权出版社提供摘要:The material removal rate, defectivity, erosion, and dishing and the effective planarization length of a CMP process depend on the local tribology (hardness, compliances) and physical properties (pore size & density, asperities) of the pad material. Graded pads exhibit spatial modulation in various material/tribological properties customized to planarize:(i) Dissimilar material stacks such as metal/barrier oroxide/nitride [STI] withminimum dishing, erosion, over polish and nanotopography.(ii) Specialized materials (low-k, strain silicon and SOI) with minimum erosion and slurry selectivity. (iii) Devices with complex design and architecture (system-on a-chip and vertical gate) with varying pattern density and chip sizes. Several types of grading described here include annular, island, step and continuous grading. The pad grading design for a CMP process for a particular slurry chemistry and wafer sweep over the pad is based on local pad material (hardness, compliances, pore size and asperities) properties. Such functionally graded polymeric pads are expected to have significant impact in planarizing scaled (sub-100 nm) silicon ICs, disk drive, micromachine (MEMs) andnanocomposite substrates.申请人:MISRA, Sudhanshu,ROY, Pradip, K.,DEOPURA, Manish 地址:US,US,US,US国籍:US,US,US,US代理机构:WHEELOCK, E., Thomas更多信息请下载全文后查看。

羊蜡酸插层制备介观层状羟基磷灰石

羊蜡酸插层制备介观层状羟基磷灰石

羊蜡酸插层制备介观层状羟基磷灰石赵大洲【摘要】羊蜡酸作为一种典型的有机脂肪酸,因具有良好的生物键合能力而受到医学界的广泛关注.本文作者在醇/水混合溶剂中,通过羊蜡酸插层制备了介观层状羟基磷灰石,并采用红外光谱、X 射线衍射以及透射电镜进行了相应的表征.分析结果显示,羊蜡酸在形成层状介观结构中起着重要的作用,所制备的样品层间距约为3.1 nm ,羊蜡酸层与羟基磷灰石层呈现交替叠加的层状结构.%As a typical organic fatty acid ,capric acid has been widely concerned in the medical community because of its good biological bonding ability .In this paper ,mesoscopic lamellar hydroxyapatite (ML-HA) was prepared by capric acid intercalation .The products were charac-terized by infrared spectroscopy ,X-ray diffraction and transmission electron microscopy .The analysis results reveal that capric acid played a decisive role in the formation of lamellar meso-structures .The lamellar spacing of the sample is about 3 .1 nm with the layered structure of capric acid layer and hydroxyapatite layer alternately superimposed .【期刊名称】《化学研究》【年(卷),期】2016(027)002【总页数】4页(P246-249)【关键词】羊蜡酸;羟基磷灰石;介观;插层【作者】赵大洲【作者单位】陕西学前师范学院化学与化工系,陕西西安 710100【正文语种】中文【中图分类】O611.4有机脂肪酸是生物机体能量来源的主要物质之一,通式为CnH2n+1COOH,在氧气充足的情况下可被氧化为二氧化碳和水,释放出大量能量,在生物医学领域有着潜在的应用价值. 除此之外,有机脂肪酸还可应用于日用化学工业中,包括化妆品、洗涤剂以及涂料等[1-4]. 羊蜡酸又叫癸酸,是一种人体必需脂肪酸,不仅在降血脂和防治冠心病方面有着重要的作用,而且还能促进儿童的生长发育和智力发育. 羟基磷灰石 (HA)是一种生物相容性较好的活性材料,被广泛应用于牙齿和骨骼的修复领域[5-12]. 介观羟基磷灰石具备可调控的纳米结构,成为近年来研究者们关注的热点. 例如,利用不同浓度的聚醚 F127 制备具有两类介观孔径尺寸的羟基磷灰石[13]. 介观羟基磷灰石的形态和结构决定了其不同的应用价值,其中层状羟基磷灰石因具有可调节的纳米级层间距而备受关注[14-15]. 本文作者在醇/水混合溶剂中,采用羊蜡酸插层,成功制备了介观层状羟基磷灰石,并进行了机理探讨.1.1 实验仪器及药品样品的红外谱图采用 Nicolet Impact-410 型 FTIR 红外光谱仪进行表征;样品的小角扫描采用 D8 FOCUS 型粉末X射线衍射仪进行表征;样品的广角扫描采用SHIMADZU XRD-6000型X射线衍射仪进行测定;采用 HITACHI H-8100 型透射电子显微镜观测样品的形貌.硝酸钙、磷酸氢二铵、氢氧化钠和无水乙醇均购自北京化工厂;羊蜡酸购自国药集团化学试剂有限公司. 以上所有化学药品均属于分析纯.1.2 实验过程样品的制备过程均在体积比为1∶1的醇水混合溶剂中进行. 配制下述3种溶液:溶液A:将 1.9 g磷酸氢二铵加入到 30 mL 醇水混合溶剂中,均匀搅拌30 min,静置,记为溶液A.溶液B:将 3.2 g 羊蜡酸和 5.9 g 硝酸钙依次加入到30 mL的醇水混合溶剂中,均匀搅拌30 min,静置,记为溶液B.溶液C:将 8 g 氢氧化钠固体溶解于100 mL 醇水混合溶剂中,均匀搅拌 30 min,记为溶液C.将溶液A与溶液B混合,持续搅拌 1 h,向混合液中加入 20 mL 溶液 C,所得混合液在 35 ℃继续搅拌 4 h后得到悬浊液,调节其 pH为 10;将反应液全部转入到 100 mL 的不锈钢反应釜中,在 100 ℃下处理1 d;所得产物经过冷却、过滤、洗涤、干燥,最终得到由羊蜡酸插层合成的介观层状羟基磷灰石,标记为 ML-HA.2.1 红外光谱分析图1是样品 ML-HA 的红外光谱图. 从图中既可以观察到羟基磷灰石的特征吸收峰,又可以观察到羊蜡酸的特征吸收峰. 其中,在 1 032 cm-1,850 cm-1 和 565 cm-1 处出现的 PO43-吸收峰与 3 150-3 650 cm-1 范围内出现的 -OH 振动峰均为羟基磷灰石的特征吸收峰. 在 1 581 cm-1 和 1 542 cm-1处出现的 -COO- 的伸缩振动峰以及在 2 950 cm-1 和 2 880 cm-1处出现的 -CHx的伸缩振动峰归属于羊蜡酸的特征吸收峰,说明羊蜡酸与羟基磷灰石已经成功复合.2.2 X射线粉末衍射谱图分析图2是样品 ML-HA 的小角X射线衍射谱图. 由图可知在2θ为2.98°、5.98°和8.96°处出现衍射峰,分别标记为 (001)、(002) 和 (003),说明样品 ML-HA 属于介观层状结构.相应的小角衍射数据见表1,依据布拉格方程λ= 2d sin θ(其中λ = 1.541 8 nm,d 为层间距,θ是布拉格角) 计算出样品 ML-HA 的周期性层间距是2.97 nm. 同时,为了进一步研究在形成介观层状结构的过程中羊蜡酸所起的重要作用,我们做了对比实验,制备出未加羊蜡酸的样品 HA,其方法与1.2相同. 图 3 是样品 ML-HA 和 HA的广角X射线衍射谱图. 二者相比较,其衍射峰位基本一致,然而HA 在小角衍射区域并未出现衍射峰. 上述实验结果说明羊蜡酸在形成介观层状结构中起着极为重要的作用.2.3 透射电镜分析透射电镜照片可以更加直观的观察到样品的微观结构. 图 4a 是样品 ML-HA 的透射电镜照片,从图中能清晰地观察到样品呈现黑白相间的层状结构,其中白色区域为羊蜡酸层,黑色区域为羟基磷灰石层,进一步说明样品 ML-HA 是羊蜡酸与羟基磷灰石交替叠加的层状结构. 图 4b 为样品 ML-HA 的高分辨透射电镜照片,从图中可以计算出样品的周期性层间距约为 3.1 nm.2.4 机理分析介观层状羟基磷灰石的形成过程属于协同模板法. 首先,在反应初期,呈现阴性的羊蜡酸与无机 Ca2+阳离子通过静电作用结合在一起;然后,在反应体系中加入 PO43- 与 OH-,使体系中的 Ca2+与 PO43-结合形成更稳定的以羊蜡酸为中间层的介观层状磷酸三钙,其介观层状结构由小角 XRD 谱图 (图5) 分析得知. 最后,经过水热处理,由图5 分析得知,样品介观层状磷酸三钙按照阴离子电荷密度和形态需求自发的重组转化为羊蜡酸层与HA层交替排列的层状结构 ML-HA. 本文作者以生物相容性较好的羊蜡酸插层制备了有序的介观层状羟基磷灰石. XRD 与TEM表征分析表明,样品层间距约为3.1 nm. 该研究成果在工业催化氧化、水质监测以及药物缓释等领域具有一定的应用前景.【相关文献】[1] SONG S K, DONG L J, CHEN S, et al. Stearic-capric acid eutectic/activated attapulgiate composite as form-stable phase change material for thermal energy storage [J]. Energy convers Manage, 201 4, 81: 306-311.[2] SAN A. Thermal reliability test of some fatty acids as PCMs used for solar thermal laten t heat storage applications [J]. Energy convers Manage, 2003, 44 (14): 2277-2287.[3] 付路军, 董发勤, 杨玉山, 等. 二元脂肪酸/SiO2 复合相变储能材料的制备与表征[J]. 功能材料, 2013, 44 (4): 1-4.[4] 陈江, 江纪修, 李炜坪. 抗癌药物载体——磁流体的制备及其性质研究[J]. 中国医院药学杂志, 1997, 17 (4): 163-166.[5] LEGEROS R. Effect of carbonate on the lattice parameters of apatite [J]. Nature, 1965, 2 06: 403-404.[6] KIKUCHI M, ITOH S, ICHINOSE S, et al. Self-organization mechanism in a bone-like hydroxyapatite/collagen nanocomposite synthesized in vitro and its biological reactio n in vivo [J]. Biomaterials, 2001, 22: 1705-1711.[7] JALOTA S, BHADURI S B, TAS A C. A new rhenanite (beta-NaCaPO4) and hydroxyapatite biophasic biomaterial for skeletal repair [J]. J Biomed Mater Res Part B, 2007, 80B: 304-316.[8] NARAYAN R J, HOBBS L W, JIN C M, et al. The use of functionally gradient materials in medicine [J]. Jom 2006, 58: 52-56.[9] WATARI F, YOKOYAMA A, OMORI M, et al. Biocompatibility of materials and developm ent to functionally graded implant for bio-medical application [J]. Compos Sci Technol, 2004, 64: 893-908.[10] FRAKENBURG E, GOLDSTEIN S, BAUER T, et al. Biomechanical and histological evaluat ion of a calcium phosphate cement [J]. Journal of Bone & Joint Surgery 1998, 80: 1112-1114.[11] YUAN H P, LI Y B, DE BRUIJN J D, et al. Tissue responses of calcium phosphate cemen t: a study in dogs [J]. Biomaterials, 2000, 21: 1283-1290.[12] THOMPSON J B, KINDT J H, DRAKE B, et al. Bone indentation recovery time correlates with bond reforming time [J]. Nature, 2001, 414: 773-776.[13] ZHAO Y F, MA J. Triblock co-polymer templating synthesis of mesostructured hydroxyapatite [J]. Micropor Mesopor M ater, 2005, 87 (2): 110-117.[14] 黄占杰. 磷酸钙陶瓷生物降解研究的进展[J]. 功能材料, 1997, 28: 1-4.[15] KASTEN P, LUGINBUHL R, VAN GRIENSVEN M, et al. Comparison of human bone mar row stromal cells seeded on calcium-deficient hydroxyapatite, beta-tricalcium phosphate and demineralized bone matrix [J]. Biomaterials, 2003, 24: 2593-2603.。

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Applied Surface Science 258 (2012) 2093–2097Contents lists available at ScienceDirectApplied SurfaceSciencej o u r n a l h o m e p a g e :w w w.e l s e v i e r.c o m /l o c a t e /a p s u scFabrication of functionally gradient nanocomposite coatings by plasma electrolytic oxidation based on variable duty cycleM.Aliofkhazraei,A.Sabour Rouhaghdam ∗Department of Materials Science,Faculty of Engineering,Tarbiat Modares University,P.O.Box:14115-143,Tehran,Irana r t i c l ei n f oArticle history:Available online 15 April 2011Keywords:Plasma electrolytic oxidation Functionally gradient coatings Nanocomposite Pulse currenta b s t r a c tPlasma electrolytic oxidation (PEO)was applied on the surface of commercially pure titanium substrates in a mixed aluminate-phosphate electrolyte in the presence of silicon nitride nanoparticles as suspension in the electrolyte in order to fabricate nanocomposite coatings.Pulsed current was applied based on vari-able duty cycle in order to synthesize functionally gradient coatings (FGC).Different rates of variable duty cycle (3,1.5and 1%/min),applied current densities (0.06–0.14A/cm 2)and concentrations of nanoparti-cles in the electrolyte (2,4,6,8and 10g l −1)were investigated.The nanopowder and coated samples were analyzed by atomic force microscope,scanning electron microscope and transmission electron micro-scope.The influence of different rates of variable duty cycle (or treatment times)on the growth rate of nanocomposite coatings and their microhardness values was investigated.The experimental results revealed that the content of Si 3N 4nanoparticulates in the layer increases with the increase of its concen-tration in the plasma electrolysis bath.Nanocomposite coatings fabricated with lower rate of variable duty cycle have higher microhardness with smoother microhardness profile.© 2011 Elsevier B.V. All rights reserved.1.IntroductionSpecial properties of micro-and nanocomposite materials [1–3]including dispersion hardening [4],self-lubrication [5],hot oxi-dation resistance [6],corrosion [7]and wear resistances [8]are different.Plasma electrolysis [9]is one of the most important methods for fabrication of micro-and nanocomposites due to precise control of the process,high deposition rate and low cost [10].Recently,a number of reports showed Si 3N 4,WC and ZrO 2nanoparticulates,which were successfully added into the plasma electrolysis bath and could be embedded with the layer to fabricate nanocomposite coatings [11].Oxide based coatings were performed as one of the surface coatings to replace hard chromium coatings for their superior properties [12],and the process has advantage of considering environmental protection [13].Among the hard ceramic based nanoparticulates used for reinforcement,silicon nitride (Si 3N 4)has been frequently studied and used for its unique properties such as high hardness,high wear resistance,good inert chemical behav-ior and high temperature properties [14].However,little work has been done about the incorporation of Si 3N 4nanoparticulates in oxide based matrix,especially with high concentration.Just one∗Corresponding author.Tel.:+989126905626;fax:+982166960664.E-mail addresses:sabour@modares.ac.ir ,sabour01@ (A.S.Rouhaghdam).report [15]has been published on the fabrication,wear and rough-ness of high concentrated Si 3N 4nanoparticulates in oxide based ceramic matrix nanocomposite layer.In this paper,Si 3N 4/TiO 2gradient nanocomposite coatings [16]were fabricated by the novel method of anodic plasma electrolysis in an aqueous based electrolyte containing Si 3N 4nanoparticulates for achieving layers with high and a gradient of concentration for nanoparticulates based on the variable duty cycle of the applied pulsed current [17].The effects of the concentration of Si 3N 4nanoparticulates in the plasma electrolysis bath and effective parameters of coating process such as current density and the rate of variable duty cycle on the amount and gradient of Si 3N 4nanoparticulates co-deposited in the nanocomposite layers were evaluated.The surface morphologies,microhardness and incorpo-ration of nanoparticles for high concentrated Si 3N 4/TiO 2gradient nanocomposite coatings were studied.2.Experimental procedureThe plasma electrolysis bath is composed of an aqueous elec-trolyte containing chemically pure sodium aluminate (15g l −1),sodium-phosphate (2g l −1)(for denser coatings)and dissolved potassium hydroxide (for reaching a desirable electrical conduc-tivity of electrolyte)mixed with Si 3N 4fine nanoparticulates.Si 3N 4nanoparticulates with the concentration range of 2–10g l −1in the electrolyte were used.A 316stainless steel electrode was used as the anode mercially pure titanium (CP-Ti)discs0169-4332/$–see front matter © 2011 Elsevier B.V. All rights reserved.doi:10.1016/j.apsusc.2011.04.0482094M.Aliofkhazraei,A.S.Rouhaghdam /Applied Surface Science 258 (2012) 2093–2097Fig.1.BF TEM image of used Si 3N 4nanopowder.(20mm Ø×5mm)were used as the cathode materials and the substrates were mechanically polished and ultrasonically cleaned in acetone for 10min.Then they were immersed without delay in the plasma electrolysis bath.Prior to the coating process,the Si 3N 4nanoparticulates (with the average size of 37nm)were immersed in the electrolyte.Fig.1illustrates the TEM bright field image of the used nanopowder.The operating plasma electrolysis condi-tions were similar to other work [15].The bath temperature was maintained constant at 25◦C by heat exchanger.The samples were biased to the rectangular-shape pulsed current generated from two power supplies [18].The frequency was maintained constant at 10kHz while the duty cycle was changed from 20%to 80%with the steps equal to 1%during the total coating time.Three differ-ent rates (3,1.5and 1%/min)were applied for changing the duty cycle.Fig.2illustrates an example of the cross-section for obtained nanocomposite coating.Phase analysis of the coatings has been done in another report [15].The surface nanostructure and the composition of Si 3N 4/TiO 2-nanocomposite layers were studied by a scanning electron microscope (SEM,Phillips XL30)equipped with energy dispersive spectrometer (EDS).Vickers microhardness tests were done on Buhler Micromet 1microhardness tester using a load of 200g,applied for 20s.The average of five measurements was reported for each microhardness value.Atomic force microscope (AFM,NanoScope II)and transmission electron microscope (TEM,CM-120FEG Philips)were used for determining the surface char-acteristics and nanostructure of the coatings and nanopowder,respectively.Fig.2.SEM micrograph of cross section for obtained nanocomposite coating.3.Results and discussionFig.3illustrates the relationship between the weight percent-age (wt.%)of the embedded Si 3N 4nanoparticulates in the surface (top layer)of the nanocomposite coatings and the concentration of the nanoparticulates in the plasma electrolysis bath at the cur-rent density of 0.045A/cm 2and the stirring rate of 100rpm.It can be said that the weight percentage of the Si 3N 4nanopartic-ulates in the nanocomposite layers increases with the increase of Si 3N 4nanoparticulates content in the plasma electrolysis bath.The embedding of Si 3N 4nanoparticulates by the plasma electrolysis method may be recognized by the adsorption of Si 3N 4nanopar-ticulates on the surface of the specimen,as studied and reported by our earlier reports [15].Variable duty cycle caused more satu-rated layer and longer coating times (lower rates for variable duty cycle)caused higher silicon concentration in the layer.Higher con-centrations of Si 3N 4nanoparticulates in the plasma electrolysis bath enhanced the adsorption rate,thus leading to a higher weight percentage of the embedded Si 3N 4nanoparticulates [19].Fig.4illustrates the effect of current density on the embedded Si 3N 4content from a bath containing 10g l −1of Si 3N 4nanopar-ticulates being stirred at 300rpm.As shown,the content of the embedded Si 3N 4nanoparticulates increases with the current density.The weight percentage of the embedded Si 3N 4nanopar-ticulates becomes approximately constant for the variable duty cycle rates higher than 1.5%/min.The increasing content of Si 3N 4nanoparticulates can be related to the increasing of embedded nanoparticulates to arrive in the surface of sample.The whole coat-ing is restricted by the adsorption of the nanoparticulates.Since the rates of variable duty cycle are higher than 1.5%/min,nanoparticu-lates have lower times to move from the electrolyte to the surface of the sample.In this case,faster plasma electrolysis process leads to fewer embedded nanoparticulates in the nanocomposite coatings [20].Fig.5illustrates the effect of different rates of variable duty cycle on the content of the embedded Si 3N 4nanoparticulates from two different baths containing 2and 6g l −1Si 3N 4nanoparticulates at current density of 0.045A/cm 2.It is shown that the rates of variable duty cycle strongly affect the weight percentage of the embedded Si 3N 4nanoparticulates,because Si 3N 4should be transported to the surface of the sample for embedding with titanium oxide ceramic matrix.The weight percentage decreases with the increasing rate of the variable duty cycle and meets a minimum value at 3%/min in this research.When the rates of variable duty cycle are high (lower coating time),the embedding behavior of Si 3N 4nanoparticulates is apparently limited by the coating time.Fig.6illustrates the AFM image of both the pure TiO 2coat-ing and the Si 3N 4/TiO 2nanocomposite layer fabricated from the plasma electrolysis bath containing 8g l −1of Si 3N 4nanoparticu-lates.It can be seen that the Si 3N 4/TiO 2nanocomposite layer has lower roughness than the pure TiO 2coating.It is evident that the embedded Si 3N 4nanoparticulates are uniformly distributed in the TiO 2ceramic based matrix by plasma electrolysis.Therefore,in order to obtain nanocomposite layers containing homogenous dis-tributed Si 3N 4nanoparticulates,it is important to well immerse the Si 3N 4nanoparticulates in the electrolyte [21].As long as the Si 3N 4nanoparticulates are uniformly distributed in the layers,the Si 3N 4/TiO 2nanocomposite coatings could show excellent mechan-ical and electrochemical properties [22].Fig.7illustrates the relationship between the microhardness profile of the gradient Si 3N 4/TiO 2nanocomposite layers and the rate of variable duty cycle.It is seen that the Si 3N 4/TiO 2nanocom-posite coating fabricated with lower rate has higher microhardness.The reason of higher microhardness of the Si 3N 4/TiO 2nanocompos-ite coatings than the TiO 2coating is that the Si 3N 4nanoparticulates,uniformly distributed in the titania based matrix,could limit theM.Aliofkhazraei,A.S.Rouhaghdam/Applied Surface Science258 (2012) 2093–20972095Fig.3.Effect of the Si3N4nanoparticulates content in the plasma electrolysis bath on the weight percentage of Si3N4in the surface of nanocomposite layers at different rates of variable duty cycle.Fig.4.Effect of the current density on the weight percentage of Si3N4nanoparticulates in the nanocomposite coatings for different rates of variable duty cycle.Fig.5.Effect of the different rates of variable duty cycle on the weight percentage of Si3N4nanoparticulates in the nanocomposite coatings.2096M.Aliofkhazraei,A.S.Rouhaghdam /Applied Surface Science 258 (2012) 2093–2097Fig.6.AFM image of the surface morphology of (a)TiO 2coating,(b)Si 3N 4/TiO 2nanocompositelayer.Fig.7.Relation between microhardness and weight percentage of embedded Si 3N 4nanoparticulates in the nanocomposite layers.growth of the TiO 2grains and the deformation of the ceramic matrix under a loading through grain polishing [23]and dispersive strengthening mechanisms [24].The grain polishing and dispersive strengthening effects get stronger as the content of Si 3N 4nanopar-ticulates in the nanocomposite layers increases,thus leading to the increased microhardness of the Si 3N 4/TiO 2nanocomposite layers.As shown in Fig.7,the microhardness profile shows three dif-ferent zones which can be studied by their microstructures and phases.As described in other paper [15],coatings show agglom-erated hard particles in the surface (top coat)while have a barrier dense layer near the coating/substrate interface.Smooth micro-hardness profile continues in the first zone with approximately a sharp decrease of microhardness in the second zone and finally shows a flat profile near the substrate [25].It is also evident that lower rates of variable duty cycle cause more smooth microhard-ness profile,which is clearly better for the load bearing ability of the coating [26].4.ConclusionsPlasma electrolysis was done successfully for fabrication of high concentrated gradient Si 3N 4/TiO 2nanocomposite layer.Embed-ding of Si 3N 4nanoparticulates in TiO 2matrix depends on the concentration of Si 3N 4nanoparticulates in the plasma electroly-sis bath,the current density and the stirring rate.The content of Si 3N 4nanoparticulates in the layer increases with the increase of its concentration in the plasma electrolysis bath.The microhard-ness of Si 3N 4/TiO 2nanocomposite layers increases with the weight percentage of the embedded Si 3N 4nanoparticulates.Si 3N 4/TiO 2nanocomposite coatings fabricated with lower rate of variable duty cycle (longer treatment times)has higher microhardness with smoother microhardness profile.The microhardness profile showed three different zones,which are related to the structure and phase distribution of the nanocomposite coatings.AcknowledgementFinancially support of Iranian nanotechnology initiative is acknowledged.References[1]V.G.Ponomareva,vrova,L.G.Simonova,Effect of SiO 2morphology andpores size 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