材料期刊网，材料期刊，材料类期刊，材料期刊投稿

A new kind of Mn-Mo-Nb-Cu-B bainite steel which satisfied mechanical demands of E690 offshore plate steel was designed. The effect of two processes——thermomechanical control process (TMCP)+tempering (T) and thermomechanical control process (TMCP)+reheating and quenching (RQ)+tempering (T)——on microstructure and mechanical properties were studied by means of scan electron microscope (SEM), transmission electron microscope (TEM) and electron back scatter diffraction (EBSD). The results showed that optimal mechanical properties were available when tempering at 550 ℃ for both processes. The microstructure of the TMCP+T treated sample tempering in the range of 450 to 550 ℃ for 1 h did not change dramatically yet the lath in the TMCP+RQ+T treated sample merged together and transformed into polygonal ferrite. At the same time, the sub-structure of grain bainite transformed from lath to cell-shape to refine grains with tempering temperature mounting. Lots of sub-grain boundaries were located within bainite and adjacent bainite grain boundaries were high angle.

关键词: offshore plate , low carbon bainitic steel , tempering , toughness , EBSD

小角度直线反走样的改进Wu算法

李铂 , 周建江 , 夏伟杰 , 吴连慧

液晶与显示 doi:10.3788/YJYXS20142904.0605

直线是机载座舱显示画面中最基本的图元,其显示质量对于整个画面的显示效果影响较大,尤其是小角度下直线显示的“麻花”现象一直是影响显示效果的关键问题之一.为了提高小角度下直线的显示效果,本文提出了一种基于Wu算法的亮度渐变改进算法.该算法通过渐进地展现直线从轴方向上的亮度变化过程,减少亮度畸变,有效地改进了显示效果.通过Matlab仿真和FPGA实现,验证了该算法反走样后的小角度直线显示效果明显优于其他算法,而且结合中点画线法后,绘制时间与Wu算法相当.同时该算法还可改善大角度直线和圆弧的显示效果,消除了大角度直线的边缘锯齿,解决了圆弧在小角度部分的虚化问题.因此本文算法可用于对实时性和显示效果要求高的机载座舱显示系统,以缓解飞行员的视觉疲劳.

关键词: 座舱显示 , 反走样 , 改进Wu算法 , 小角度 , FPGA实现

基于Wu反走样的三角形光栅化边缘反走样算法

吴连慧 , 周建江 , 夏伟杰 , 陈雅雯

液晶与显示 doi:10.3788/YJYXS20153001.0163

对于光栅化的三角形,其边缘存在明显的锯齿现象,因此需要进行反走样处理.基于Wu直线反走样算法的思想,考虑了水平直线外侧直接添加插值点的算法和三角形三边外侧反走样的算法.综合两者的优点,在绘制光栅化的三角形的同时,边缘叠加Wu反走样直线,并考虑背景像素灰度值的作用.结果表明,改进的三角形光栅化的边缘反走样算法有效提高了三角形光栅化后边缘的显示效果,该算法计算量小,便于FPGA实现,可用于对图形显示质量要求很高的机载显示系统.

关键词: 反走样 , Wu算法 , 光栅化 , FPGA

碳酸钙粒子增韧高密度聚乙烯的脆韧转变——Wu氏增韧理论聚合物共混物脆韧转变判据的适用条件

胡跃鑫 , 冯玉林 , 姜伟

应用化学 doi:10.3724/SP.J.1095.2011.00521

采用不同尺寸的碳酸钙粒子增韧高密度聚乙烯,研究了不同温度下共混体系的临界粒子间距与碳酸钙粒子尺寸和含量之间的关系,确定了温度是Wu氏增韧理论临界粒子间判据适用性的重要影响因素.结果表明,在17℃下,临界粒子间距与碳酸钙粒子的尺寸和含量无关,该条件下Wu氏增韧理论临界粒子间距判据是适用的;而随着温度的升高,发现临界粒子间距依赖于碳酸钙粒子的尺寸,表明高温条件下,Wu氏增韧理论临界粒子间距判据不再适用.

关键词: 聚合物增韧 , 粒子间距 , 脆韧转变

CaYO(BO3)3晶体坩埚下降法生长

罗军 , 钟真武 , 范世(马豈) , 王锦昌

人工晶体学报 doi:10.3969/j.issn.1000-985X.2000.01.005

本文首次报道了Ca4YO(BO3)3(YCOB)晶体的坩埚下降法生长.在1600～1650℃炉温下,固液界面处的纵向温度梯度为40～60℃/cm,以0.2～0.6mm/h的生长速率,在近封闭的Pt坩埚中生长出了直径达25mm、长度超过50mm的完整透明YCOB晶体.介绍了生长工艺和原料制备,观察发现晶体中的主要宏观缺陷是包裹体.分析了包裹体生成的原因.

关键词: 布里奇曼法 , Ca4YO(BO3)3晶体 , 非线性光学材料 , 包裹体

Synthesis, structure and magnetic properties of Fe-Gd nanocapsules coated with B2O3/H3BO3 and Fe3BO5+GdBO3

Physica B-Condensed Matter

Nanocapsules consisting of B2O3/H3BO3 encapsulating Fe-Gd cores have been synthesized by an arc-discharge process using metal-boron alloys as cathode. Most of the nanocapsules have a well-constructed shell/core structure with a uniform B2O3/H3BO3 shell. Heat-treatment induces reactions between the shell and the core, resulting in the formation of a Fe3BO5+GdBO3 matrix embedded with Fe nanoparticles, reduction of the metallic-core size and decrease of the blocking temperature T-B. Above T-B, the magnetization curves plotted vs. H/T overlap and show zero coercivity. Below T-B, the coercivity shows a linear dependence when plotted vs. T-1/2. However, the coercivity-T-1/2 curve below 60 K has a different slope from that above 60 K, indicating the existence of two different magnetic phases in the nanocapsules. Different from bulk Fe3BO5, nanoscale Fe3BO5 particles have a lower transition temperature to the weak-ferromagnetic state. and magnetic hysteresis is absent due to size effects. (C) 2004 Elsevier B.V. All rights reserved.

关键词: nanocapsules;transmission electron microscopy (TEM);X-ray;photoelectron spectroscopy (XPS);magnetic properties;arc-discharge;boric-acid;boron;carbon;oxide;nanoparticles;particles;diborane;iron

Na3La9O3(BO3)8的晶体结构

张国春 , 傅佩珍 , 李云阁 , 吴以成

人工晶体学报 doi:10.3969/j.issn.1000-985X.2005.05.001

以Na2CO3-H3BO3为助熔剂,用顶部籽晶法生长出Na3La9O3(BO3)8单晶.测定了Na3La9O3(BO3)8晶体结构,结果表明:该晶体属六方晶系,空间群:P62m,晶胞参数为a=b=0.89229(13)nm,c=O.87366(17)nm,α=β=90°,γ=120°,Z=1,V=0.60240(17)nm3,密度为5.066g/cm3.晶体结构中的硼氧基团是平面的BO3基团,BO3基团相互独立,通过与Na(1)O6、La(1)O9和La(2)O8的配位多面体连结形成层状结构,所有层平行于(001)面.描述了Na3La9O3(BO3)8晶体在非线性光学材料领域的应用前景.

关键词: Na3La9O3(BO3)8 , 晶体结构 , 倍频效应

Na3La2(BO3)3的晶体结构

张国春 , 李云阁 , 傅佩珍 , 潘世烈 , 常峰 , 吴以成

人工晶体学报 doi:10.3969/j.issn.1000-985X.2004.04.007

以Na2CO3-H3BO3-NaF为助熔剂,使用顶部籽晶法生长出Na3La2(BO3)3透明单晶.测定了Na3La2(BO3)3的晶体结构,该晶体属正交晶系,空间群:mm2(No.38),晶胞参数为a＝0.51580(10)nm,b=1.1350(2)nm,c=0.73230(15)nm,α＝β＝γ＝90°,V＝0.42871(15)nm3,密度:.053g/cm3.晶体结构中的硼氧基团是平面的BO3基团,BO3基团相互独立,且与Na(1)O6、Na(2)O8、Na(3)O6和La(1)O9配位多面体连结形成三维网络骨架结构.讨论了Na3La2(BO3)3的晶体结构与倍频效应的关系.

关键词: Na3La2(BO3)3 , 晶体结构 , 倍频效应

Ba7(BO3)3F5晶体结构及热分析

刘剑

人工晶体学报

采用高温溶液法从BaCO3,BaF2及H3BO3混合体系中生长出了一种氟硼酸钡晶体,Ba7(BO3)3F5晶体属六方晶系,空间群为P63mc,晶胞参数:a=1.11562(15) nm,c=0.72415(14) nm,Z=2,V=0.7805(2) nm3.Ba7(BO3)3F5晶体结构是由Ba(1)O7F3基团,Ba(2)O4F3基团,Ba(3)O6F4基团和独立的BO3基团相互连接形成的三维空间网络结构.Ba7(BO3)3F5的热分析分析结果表明Ba7(BO3)3F5在1070℃同成份熔化.

关键词: Ba7(BO3)3F5 , 晶体结构 , 高温溶液法