石墨烯/铁氰化钴复合膜修饰玻碳电极同时测定对苯二酚、邻苯二酚和间苯二酚

采用滴涂法和电沉积法制备了石墨烯/铁氰化钴复合膜修饰玻碳电极. 用扫描电镜对该纳米复合膜进行了表征.用循环伏安法研究了对苯二酚(HQ)、邻苯二酚(CT)和间苯二酚(RS)在修饰电极上的电化学行为. 实验结果表明, 相对于裸玻碳电极和石墨烯修饰电极, HQ, CT 和RS 在石墨烯/铁氰化钴修饰电极上的氧化峰电流显著提高. 利用差分脉冲伏安法测定, HQ, CT 和RS 分别在1.0×10^－6～1.5×10^－4 mol/L, 1.0×10^－6～2.0×10^－4 mol/L 和3.5×10^－6～2.5×10^－4 mol/L浓度范围内与氧化峰电流呈良好的线性关系, 相关系数分别为0.991, 0.993 和0.992. 信噪比为3 时, HQ, CT 和RS 检出限分别为2.0×10^－7, 2.1×10^－7 和3.5×10^－7 mol/L. 将该方法用于水样分析, 回收率为95.6%～106.1%.     

电喷雾串联质谱中苯乙酰苯胺衍生物去质子化离子裂解产生阴离子自由基的机理研究

电喷雾串联质谱中偶电子负离子裂解产生阴离子自由基是一种违反偶电子规则的异常碎裂反应, 但是这种碎裂反应也常常被观察到, 其机理传统上一直被认为是共价键的简单均裂. 针对苯乙酰苯胺及其衍生物(R¹C₆H₄CH₂CONH- C₆H₄R²)的去质子化离子([M-H]^-)裂解生成阴离子自由基这一特殊的碎裂反应提出了一个新颖的反应机理, 即离子/中性复合物介导的单电子转移反应机理. 以化合物3 (R¹＝H, R²＝NO₂)为模型提出的反应机理为, 首先氮上负电荷诱导CH₂—CO键异裂生成[苄基负离子/4-硝基苯异氰酸酯]复合物中间体, 然后复合物中发生单电子转移反应产生4-硝基苯异氰酸酯阴离子自由基. 通过取代基效应研究(电子亲和势分析)、与文献报道的双分子电子转移反应比较和密度泛函理论计算等方法, 新反应机理得到了证明.     

A multiscale material point method for impact simulation

To better simulate multi-phase interactions involving failure evolution, the material point method (MPM) has evolved for almost twenty years. Recently, a particle-based multiscale simulation procedure is being developed, within the framework of the MPM, to describe the detonation process of energetic nano-composites from molecular to continuum level so that a multiscale equation of state could be formulated. In this letter, a multiscale MPM is proposed via both hierarchical and concurrent schemes to simulate the impact response between two microrods with different nanostructures. Preliminary results are presented to illustrate that a transition region is not required between different spatial scales with the proposed approach.     

An oscillator using high order Lamb wave modes

An oscillator using high order Lamb wave modes is presented. Due to the multimode property of Lamb waves, high frequency oscillators using high order mode Lamb waves can be fabricated. To select the operating mode of the Lamb wave oscillator, a high order mode selector is inserted into the feedback loop. An oscillator using the 13th antisymmetric mode (a₁₃) in Lamb wave is achieved in experiments and the oscillating frequency is 5.30 times higher than that of the a₀ mode excited by the interdigital transducer.     

色散缓变光纤中初始啁啾对超高斯脉冲传输特性的影响

从非线性薛定谔方程出发,采用变分法,导出了色散缓变光纤中超高斯脉冲参数随传输距离的演化方程组及其解,讨论了初始啁啾对色散缓变光纤中超高斯脉冲传输特性的影响.求出了振幅与脉宽、频率与啁啾、脉宽与啁啾之间的三个解析约束关系,得出了脉宽随传输距离演化的解析解,用龙格-库塔法进行数值求解描绘了初始啁啾和脉冲前后沿锐度对呈指数变化的色散缓变光纤中超高斯脉冲的脉宽的影响.结果表明:初始嘣啾、色散缓变和脉冲前后沿锐度对超高斯脉冲的振幅、脉宽、唰啾和相位有直接影响,脉冲前后沿锐度对超高斯脉冲中心位置没有影响,超高斯脉冲传输过程中会产生唰啾,但脉冲中心的等效频率保持为常数.     

偶氮金属螯合物薄膜的光学常数和吸收光谱

偶氮金属螯合物薄膜是一类新型光信息存储和光学非线性材料。通过旋涂法在单晶硅上制备了三种新型偶氮染料：2-（4-甲革-2-噻唑基偶氮）-5-二乙基胺苯酚（MTADP）掺杂聚合物,MTADP的镍螯合物（Ni-MTADP）和锌螯合物（Zn-MTADP）薄膜。利用宽谱扫描全自动椭圆偏振光谱仪测定了上述薄膜的椭偏光谱,获得了三种薄膜在400—700nm波段的复折射率、复介电常量和吸收系数。两种金属螯合物薄膜的共振波长比非螯合物薄膜红移了60—70nm;光学常数和吸收系数在峰值的数值也发生了明显的变化。由于这两种螯合物具有不同的立体结构,Ni-MTADP薄膜的共振波长比Zn-MTADP有10nm的红移。     

自然循环预冷和低温热管耦合系统的初步实验研究

介绍的高效低温传热方法主要包括 :自然循环冷却法和基于自然循环预冷及低温热管的高效低温冷却方法。自然循环冷却法的特点是在大温差条件下实现物体的快速冷却。一旦被冷却物体到达或接近低温液体的温度 ,将产生循环动力不足的情况 ,必须采用诸如气体引射或容器自增压等方法加以解决。而低温热管的特点在于能在小温差条件下 ,传递大量的热能。文中将自然循环预冷法及低温热管技术有机结合 ,综合自然循环和低温热管的优点 ,取长补短 ,既可以在很短的时间内使被冷却物体的温度降低下来 ,又可以保证被冷却物体的温度波动较小。文中还详细给出了基于自然循环预冷及低温热管的高效低温传热单元的设计及试验结果     

Leucolusine, a tetracyclic alkaloid with a novel ring system incorporating an oxindole moiety and fused piperidine-tetrahydrofuran rings

A tetracyclic ring-opened oxindole alkaloid, possessing an unprecedented ring system incorporating fused piperidine-tetrahydrofuran rings, has been isolated from the Malayan species, Leuconotis griffithii. The structure was established by analysis of the spectroscopic data and a possible biogenetic pathway from an Aspidosperma precursor is presented.     

Dual template approach for the synthesis of hierarchically mesocellular carbon foams

We demonstrated a simple and effective dual-templating approach for the synthesis of hierarchically mesocellular carbon foams by using nonionic surfactant of sorbitan monooleate and silica colloid particles as sacrificial templates, and resorcinol/ formaldehyde as carbon source. The representative carbon foam has dual mesopore sizes of 4 and 10 nm, and possesses the specific surface area of 580 m2/g and the total pore volume of 0.80 cm3/g.     

Size effect of fullerene cages and encaged clusters in M<Subscript>3</Subscript>N@C<Subscript>2<Emphasis Type="Italic">n</Emphasis></Subscript>

Based on the calculated findings that the sizes of encaged clusters determine the structures and the stability of C₈₀-based trimetallic nitride fullerenes (TNFs), more extensive density functional theory calculations were performed on M₃N@C₆₈, M₃N@C₇₈ and M₃N@C₈₀ (M=Sc, Y and La). The calculated results demonstrated that the structures and stability undergo a transition with the increasing of the sizes of the cages and clusters. Sc₃N is planar inside the three considered cages, Y₃N is slightly pyramidal inside C₆₈-6140 and C₇₈-5 and planar inside I_h C₈₀-7, however, La₃N is pyramidal inside all the three cages. Those cages with pyramidal clusters inside deformed considerably, compared with their parent cages. In these cases, the bonding of metallic atoms toward the cages does not play an important role, and the encaged cluster tends to be located inside the cages with the largest M-M and M-C distances so that the strain energy can be released mostly. These calculations revealed the size effect of fullerene cages and encaged clusters, and can explain the position priority of M3N inside fullerene cages and the differences in yield of M₃N@C_2n . Supported by the Southwest University, China (Grant No. SWNUB2005002)