面向装配节点平衡的产品生产物流协调优化研究

在由多个并行零件生产线和装配线组成的产品生产物流中, 各生产线的瓶颈工序制约了装配节点及其整个生产物流的平衡. 为此, 基于约束理论和JIT(Just In Time)思想, 提出主、次瓶颈的概念及其判别方法和主瓶颈拉动次瓶颈、瓶颈前后拉动生产与平行顺序移动生产相结合的生产策略, 研究了基于负荷率的瓶颈工序负荷控制方法和主瓶颈触发次瓶颈拉式生产的时间控制方法, 使瓶颈工序利用率最大化, 各个零件到达装配节点的同步性得到改善. 算例的SIMIO仿真结果表明, 装配节点的在制品存量大幅度减少, 利用率提高.     

若干高维可积和不可积模型的严格解

可积和不可积模型可以描述自然科学中的诸多现象, 寻找高维非线性模型的严格解已成为可积系统的一个重要研究内容. 结合达布变换法和多线性分离变量法, 可以得到多个(2+1)维非线性模型包含任意函数的严格解, 通过选取不同的任意函数, 构造这些非线性模型新的相互激发模式. 进一步推广了形变映射理论, 建立了变系数 场和sine-Gordon以及双sine-Gordon场的形变映射关系, 从而得到高维不可积模型包含任意函数的新严格解. 对任意函数的不同选择, 构造了sine-Gordon和双sine-Gordon可积模型丰富的局域解和周期解, 如多solitoff解及其周期波推广、周期形变的蛇形孤波解以及变模的拟周期解等.     

对称理论在解若干非线性问题中的应用

将摄动理论和对称约化理论结合起来对研究扰动非线性方程具有重要的意义. 本文利用近似对称约化理论研究了扰动mKdV方程, 得到了该方程的各阶近似约化方程和级数约化解. 本文还讨论了同伦近似对称方法在求解不可积系统中的应用以及利用对称和守恒律的关系求解非线性系统的无穷多守恒律等问题.     

通过Painlevé分析从低维模型中寻找高维可积模型

将Painlevé方法推广到更一般的形式, 可以从给定的低维可积模型中得到无穷多个新的可积模型. 新的可积模型与原模型相比都是较高维的, 它们保持保角不变性和Painlevé性质. 本文主要以KdV、NLS和KP方程为例, 运用WTC法、截断展开、领头项分析等方法, 给出了(3+1)维可积模型的具体形式.     

Strong Pauli paramagnetic effect in the upper critical field of KCa2Fe4As4F2

Recently, 12442 system of Fe-based superconductors has attracted considerable attention owing to its unique double-Fe As-layer structure. A steep increase in the in-plane upper critical field with cooling has been observed near the superconducting transition temperature, Tc, in KCa2Fe4As4F2 single crystals. Herein, we report a high-field investigation on upper critical field of this material over a wide temperature range, and both out-of-plane(H∥c, Hc2c) and in-plane(H∥ab, Hc2ab ) directions have been measured.A sublinear temperature-dependent behavior is observed for the out-of-plane Hc2c , whereas strong convex curvature with cooling is observed for the in-plane Hc2ab . Such behaviors could not be described by the conventional Werthamer-Helfand-Hohenberg(WHH) model. The data analysis based on the WHH model by considering the spin aspects reveals a large Maki parameter α=9,indicating that the in-plane upper critical field is affected by a very strong Pauli paramagnetic effect.     

Multiple bright and dark soliton solutions in three component spinor Bose-Einstein condensates

We investigate a quasi one dimensional spin-1 Bose-Einstein Condensates (BEC) in the absence of an external confinement governed by a system of three coupled Gross-Pitaevskii (GP) equation. Based on the Lax-pair, we construct one soliton solution employing gauge transformation method. In addition, the multiple bright and dark soliton solutions are obtained by properly choosing amplitude dependent parameter in the Lax-pair. The results of the paper emphasizes the richness in the structure of soliton solutions admitted by the spin components, a phenomenon which has never been brought out to the fore. We have also extended the gauge transformation method to generate two soliton solutions.     

环化顺1，4－聚丁二烯浓溶液的流动行为

大多数线型高聚物浓溶液的流动行为呈现非牛顿性，线型顺１，４－聚丁二烯（ＬＢＲ）亦然，而环化顺１，４－聚丁烯（ＣＢＲ）的浓溶液在浓度达１７．８％时仍表现为牛顿流体。ＣＢＲ溶液的临界缠结浓度明显地高于ＬＢＲ，ＣＢＲ分子链间的缠结效应比ＬＢＲ弱得多，这是ＣＢＲ的分子链结构特征所致。     

低碳醇合成Raney Cu－Co催化剂的表征

本文采用ＸＲＤ、ＸＰＳ、及Ｈ_２—ＴＰＤ技术对不同Ｃｕ／Ｃｏ比的几个ＲａｎｅｙＣｕ－Ｃｏ催化剂进行了表征．并与反应醇选择性进行了关联．结果表明：ＲａｎｅｙＣｕ－Ｃｏ催化剂均由不同Ｃｕ／Ｃｏ比的两个Ｃｕ－Ｃｏ固溶体相组成，还原（Ｈ_２，５６３Ｋ，２ｈ）前，表面除有Ｃｕ￣０和Ｃｏ￣０外，尚有少量Ｃｕ￣（＋１）和显著量的Ｃｏ￣（＋２）存在，还原后，Ｃｕ￣（＋１）几乎消失，Ｃｏ￣（＋２）仍有一定量存在，在反应温度下（５６３Ｋ），ＣＯ和ＣＯ_２均能使表面Ｃｏ￣０部分氧化，且ＣＯ_２氧化能力大于ＣＯ，而合成气（Ｈ_２／ＣＯ＝２）表现为还原的性质。三种气氛对Ｃｕ￣０无明显影响。催化剂表面Ｃｕ／Ｃｏ比高于体相Ｃｕ／Ｃｏ比，表面Ｃｕ富集显著．ＲａｎｅｙＣｕ－Ｃｏ催化剂表面有四种吸氢中心：Ｃｕ（弱吸氢中心），高配位Ｃｏ（弱吸氢中心），低配位Ｃｏ（活化吸氢中心），及强吸氢中心；对不同催化剂，表面低配位Ｃｏ中心的比例与醇选择性有一致的变化规律。基于上述结果，就ＣＯ播入中心进行了讨论。     

有机成分标准物质的研究

列出了国家标准物质研究中心最近研制的有机成分标准物质。高纯度、定值准确可靠、良好的溯源性和系列性是这些标准物质的特点。对其应用作了介绍,并指出了将来的研究方向。     

固溶体结构对Ca2-xSrxZn4Ti15O36∶Pr3+发光性质的影响

Ca_2-xSr_xZn₄Ti₁₅O₃₆∶Pr red long decay phosphor was synthesized by high temperature solid state reaction. Photoluminescence property and crystalline and unit cell parameters of the orthorhombic were investigated by fluorescence spectrophotometer and by powder X-ray diffraction, respectively. The emission intensity at 618 nm changes sharply when the concentration of Sr²⁺ (x) is less than 0.1 and the emission intensity reaches the maximum when x is equal to 0.007. There is an obviously broad excitation band at 270 nm when x is equal to 0.003 and it disappears gradually when x is over 0.01. The unit cell a parameter of Ca_2-xSr_xZn₄Ti₁₅O₃₆∶Pr decreases while c parameter increases with the increases of the concentration of the doped Sr²⁺. When x is over 0.1 the value of the unit cell parameters a and c become stable. TL peaks of Ca₂Zn₄Ti₁₅O₃₆∶Pr, Ca_1.993Sr_0.007Zn₄Ti₁₅O₃₆∶0.002Pr³⁺, 0.002Na⁺, are located at 62 ℃, 88 ℃, respectively, which indicates that there are deeper traps in Ca_1.993Sr_0.007Zn₄Ti₁₅O₃₆∶0.002Pr³⁺, 0.002Na⁺.