公交车,你等等我!

急匆匆地吃完早餐,以百米冲刺的速度跑到公交车站牌……可结果竟然是——错过公交车!然后,等啊等,感觉自己等了几个世纪,可还没见到公交车的影子.哎呀,怎么车子还没来呀?我赶时间呢!眼看着时间一分分过去,让人抓狂得想直接奔跑.     

基于CPLD的液晶驱动板的设计与实现

本文设计并实现了一种基于复杂可编程逻辑器件的液晶显示屏驱动板.采用“可编程逻辑器件+存储器”的设计方案,将存储器中的数据与液晶屏上的点一一对应.通过对系统方案的分析,设计了时钟模块、接口数据转换模块、存储器模块以及显示模块.使用硬件描述语言编程实现了各个模块的功能,并在QuartusⅡ软件平台上进行了仿真验证,最后下载...     

完全发展的非对称槽道湍流的分形维数研究

湍流的分形维数刻画了湍流的统计正则性 ,本文利用正交子波变换对完全发展的非对称槽道湍流脉动速度的实验数据进行了分析研究。文中首先将脉动速度信号分解到各个尺度 ,然后利用正则法和盒子法两种方法计算了不同尺度信号的分形维数 ,着重于考虑分形维数的变化趋势。研究结果表明 :(1 )随着信号分解尺度的增加 ,速度信号的低频部分和高频部分的维数都逐渐减小 ;(2 )逆输运现象对速度信号的分形维数没有本质的影响 ;(3)正则法计算得到的分形维数要略大于盒子法得到的分形维数     

SCALING EXPONENTS IN FULLY DEVELOPED ASYMMETRIC CHANNEL FLOW

IntroductionDuetotheimportanceofglobalandlocalscalingexponents,theyattractmanyturbulentresearchersduringthepasttwentiesyears.Butresultsobtaineduptonowaremainlyonisotropicturbulence ,bothinexperimentsandnumericsimulations[1].Itisfoundthatξpisnonlinearfunc…     

低成本基板倒装焊底充胶分层裂缝扩展研究

采用MIL-STD-883C热循环疲劳加载标准，通过电学检测方法测定了B型和D型两种倒装焊封装焊点寿命。并使用无损声学C-SAM高频超声显微镜技术观测这两种倒装焊封装在焊点有无断裂两种情况时芯片／底充胶界面的分层和扩展，计算得到分层裂缝扩展速率。在有限元模拟中采用粘塑性和时间相关模量描述了SnPb焊点和底充胶的力学行为。使用裂缝尖端附近小矩形路径J积分方法作为断裂力学参量得到不同情况下的界面分层裂缝顶端附近的能量释放率。然后由实验裂缝扩展速率和有限元模拟给出的能量释放率得到可作为倒装焊封装可靠性设计依据的Par—is半经验方程。     

The Origin and Mathematical Characteristics of the Super-Universal Associated-Legendre Polynomials

We study the mathematical characteristics of the super-universal associated-Legendre polynomials arising from a kind of double ring-shaped potentials and obtain their polar angular wave functions with certain parity. We find that there exists the even or odd parity for the polar angular wave functions when the parameter η is taken to be positive integer, while there exist both even and odd parities when η is taken as positive non-integer real values. The relations among the super-universal associated-Legendre polynomials, the hypergeometric polynomials, and the Jacobi polynomials are also established.     

LuTaO$lt;sub$gt;4$lt;/sub$gt;相变及结构

LuTaO₄是最高密度的闪烁体基质, 研究它的结构及其相变对单晶制备具有指导意义. 用固相法制备了Lu₂O₃和Ta₂O₅摩尔比为1:1时在不同温度下形成的多晶粉末, 用X射线衍射及Rietveld全谱拟合研究了多晶粉末的物相和结构. 结果表明, Lu₂O₃: Ta₂O₅摩尔比为1:1的样品在1740 ℃时合成的物相为M'-LuTaO₄, 在1800 ℃时为M'-LuTaO₄和M-LuTaO₄的混合物, 在1840 ℃时全部转变为M-LuTaO₄. 当温度升高到2058 ℃时, 样品呈熔融状态, 对淬火得到的样品进行结构精修, 给出了M-LuTaO₄, Lu₃TaO₇和Ta₂O₅的晶胞和原子坐标参数, 它们的重量比分别占78.1%, 18.9%和3.0%. 这些结果为制备以LuTaO₄为基质的高密度闪烁体单晶具有参考价值. 关键词： 4')" href="#">LuTaO₄ 相变 粉末衍射 Rietveld精修     

透明β-NaYF_4∶Yb,Tm/PMMA纳米复合材料的制备及其光学性能

采用高温溶剂热法制备了一系列不同Yb3+掺杂浓度的上转换发光纳米粒子β-NaYF4∶Yb,Tm和核壳结构的β-NaYF4∶Yb,Tm@β-NaYF4∶Yb纳米粒子。采用X射线衍射(XRD)、场发射扫描电镜(FESEM)、光致发光(PL)谱对材料的物相结构、形貌特征和发光性质进行了表征和研究,并特别研究了温度对材料发光性能的影响。结果表明:保持Tm3+浓度不变,随着Yb3+掺杂浓度的增加,β-NaYF4∶Yb,Tm的发光强度先增大后减小。当Yb3+掺杂摩尔分数为30%时,474 nm和645 nm处的发光强度达到最大值;当Yb3+掺杂摩尔分数为50%时,450 nm和692 nm处的发光强度达到最大值。在β-NaYF4∶Yb(30%),Tm上包裹一层β-NaYF4∶Yb壳层后,其发光显著增强,随壳层Yb3+摩尔分数的增加,发光强度也是先增大后减小。当壳层Yb3+摩尔分数为10%时,核壳结构纳米粒子的发光强度达到最大值;当壳层Yb3+摩尔分数达到40%时,核壳结构纳米粒子的发光强度已经低于未包裹时。将样品进行热处理后,荧光增强。样品的发光强度随环境温度的升高,红光变弱,蓝光增强。采用原位聚合法将β-NaYF4∶Yb,Tm纳米粒子与PMMA制成复合材料后,仍能保持较好的透明度和发光强度。     

Sm1 xMx(TTA)3phen转光剂的合成及荧光性能

采用化学沉淀法合成了具有紫外转红光性能的转光剂Sm1 xMx(TTA)3phen (M=Y,Gd).借助红外光谱、紫外 可见光吸收光谱及荧光光谱对配合物的性能进行了表征.结果表明:Sm1 xMx(TTA)3phen与Sm(TTA)3phen的配位结构基本一致|配合物的紫外光吸收特性主要由有机配体决定|配合物吸收紫外光后,均发出Sm3+的特征光,其中Sm0.5Y0.5(TTA)3phen在647 nm处的荧光强度在配合物中最强,达到9.5×106 cps|敏化离子的掺入可以提高配合物的荧光强度,荧光增强效果Y3+优于Gd3+.     

Longitudinal and transverse structure functions in decaying nearly homogeneous and isotropic turbulenceLongitudinal and transverse structure functions in decaying nearly homogeneous and isotropic turbulenceLongitudinal and transverse structure functions in decaying nearly homogeneous and isotropic turbulence

Streamwise evolution of longitudinal and transverse velocity structure functions in a decaying homogeneous and nearly isotropic turbulence is reported for Reynolds numbers Re;t up to 720. First, two theoretical relations between longitudinal and transverse structure functions are examined in the light of recently derived relations and the results show that the low-order transverse structure functions can be well approximated by longitudinal ones within the sub-inertial range. Reconstruction of fourth-order transverse structure functions with a recently proposed relation by Grauer et al. is comparatively less valid than the relation already proposed by Antonia et al. Secondly, extended self-similarity methods are used to measure the scaling exponents up to order eight and the streamwise evolution of scaling exponents is explored. The scaling exponents of longitudinal structure functions are, at first location, close to Zybin＇s model, and at the fourth location, close to She-Leveque model. No obvious wend is found for the streamwise evolution of longitudinal scaling exponents, whereas, on the contrary, transverse scaling exponents become slightly smaller with the development of a steamwise direction. Finally, the stremwise variation of the order-dependent isotropy ratio indicates the turbulence at the last location is closer to isotropic than the other three locations.