Promising activated carbons derived from cabbage leaves and their application in high-performance supercapacitors electrodes

In this paper, cabbage leaves (CLs) were used to synthesize porous activated carbon by the carbonization and activation processes. The material for CLs were carbonized at 600 °C and activated at 800 °C with the KOH/C-600 mass ratio 4 (denoted as AC-800) show typical amorphous character and display porous structures with high specific surface areas 3102 m²/g via XRD and BET measurements. As the electro-active material, AC-800 electrode exhibit ideal capacitive behaviors in aqueous electrolytes and the maximal specific capacitance is as high as 336 F/g at the current density of 1 A/g. Furthermore, AC-800 electrode shows excellent electrochemical cycle stability with ～95 % initial capacitance being retained after 2000 cycles. The desirable capacitive performances enable the CLs to act as a new biomass source of carbonaceous materials for high-performance supercapacitors and low-cost electrical energy storage devices.     

Do coupling exciton and oscillation of electron-hole pair exist in neutral and charged pi-dimeric quinquethiophenes?

Optical physical properties of neutral and charged quinquethiophene monomer, and neutral and cationic pi-dimeric quinquethiophenes were investigated with density functional theory as well as the two dimensional (2D) site (transition density matrix) and three dimensional (3D) cube (transition density and charge difference density) representations, stimulated by the recent experimental report [T. Sakai et al., J. Am. Chem. Soc. 127, 8082 (2005)]. Transition density shows the orientation and strength of the transition dipole moment of neutral and charged quinquethiophene monomer, and charge difference density reveals the orientation and result of the charge transfer in neutral and charged quinquethiophene monomer. To study if coupling exciton and oscillation of electron-hole pair exist in neutral and cationic pi-dimeric quinquethiophenes, the coupling constants J (coupling exciton of electron-hole pair) and K (coupling oscillation of electron-hole pair) were introduced to the exciton coordinate and momentum operators, respectively, and the 2D and 3D analysis methods were further developed by extending our previous theoretical methods [M. T. Sun, J. Chem. Phys. 124, 054903 (2006)]. With the new developed 2D and 3D analysis methods, we investigated the excited state properties of neutral and cationic pi-dimeric quinquethiophenes, especially on the coupling exciton and oscillation of electron-hole pair between monomers. The 2D results show that there is neither coupling exciton (J=0) nor oscillation (K=0) of electron-hole pair in neutral pi-dimeric quinquethiophenes. For some excited states of cationic pi-dimeric quinquethiophenes, there is no coupling exciton (J=0), but there is coupling oscillation (K not equal0); while for some excited states, there are both coupling exciton and coupling oscillator simultaneously (J not equal0 and K not equal0). The strength of transition dipole moments of pi-dimeric quinquethiophenes were interpreted with 3D transition density, which reveals the orientations of their two subtransition dipole moments. The 3D charge transition density reveals the orientation and result of intermonomer and/or intramonomer charge transfer. The calculated results reveal that excited state properties of neutral pi-dimeric quinquethiophene are significantly different from those of the cationic pi-dimeric quinquethiophenes.     

Lipschitz强增殖映射方程的迭代解

本文讨论一致凸Banach空间中的Lipschitz强增殖映射方程解的Ishikawa迭代和Mann迭代的收敛性,部分回答了Chianme提出的两个问题。     

一种静电像管优化设计方法的设想

从数值计算出发,以实例计算静电像管的均方根半径值,给出系统在最佳像面及其各附加像面处的均方根值,验证了理论分析的正确性,并从理论上提出了一种关于静电像管优化设计方法的设想。     

Photo-Induced Self-assembly of Copolymer-Capped Nanoparticles into Colloidal Molecules

Colloidal molecules (CMs) are precisely defined assemblies of nanoparticles (NPs) that mimic the structure of real molecules, but externally programming the precise self-assembly of CMs is still challenging. In this work, we show that the photo-induced self-assembly of complementary copolymer-capped binary NPs can be precisely controlled to form clustered AB _x or linear ( AB ) _y CMs at high yield (x is the coordination number of NP- B s, and y is the repeating unit number of AB clusters). Under UV light irradiation, photolabile p-methoxyphenacyl groups of copolymers on NP- A *s are converted to carboxyl groups (NP- A ), which react with tertiary amines of copolymers on NP- B to trigger the directional NP bonding. The x value of AB _x can be precisely controlled between 1 and 3 by varying the irradiation duration and hence the amount of carboxyl groups generated on NP- A s. Moreover, when NP- A * and NP- B are irradiated after mixing, the assembly process generates AB clusters or linear ( AB ) _y structures with alternating sequence of the binary NPs. This assembly approach offers a simple yet non-invasive way to externally regulate the formation of various CMs on demand without the need of redesigning the surface chemistry of NPs for use in drug delivery, diagnostics, optoelectronics, and plasmonic devices.     

聚奥-9C装药的传爆管殉爆

为了研究冲击波作用下引信传爆装置的响应规律,进行了以主发炸药为RDX-8701、被发装置为聚奥-9C（JO-9C）装药的传爆管（含导爆药柱）的殉爆实验。通过观测残留传爆药、壳体和见证块变形,判断传爆管的爆炸程度,分析了殉爆过程中JO-9C爆轰波的成长历程及传播规律。采用AUTODYN软件建立了殉爆实验有限元模型,计算模型中主要考虑了主发炸药产生的爆炸冲击波对传爆管的冲击响应。基于流固耦合方法,通过调整距离模拟计算得到了传爆管的临界殉爆距离和殉爆安全距离。结果表明,传爆管上端的侧角受到爆炸冲击后产生的爆轰波沿斜下方传播,使传爆药柱完全爆轰,并引起导爆药柱发生殉爆;数值模拟结果显示,JO-9C装药的传爆管临界殉爆距离为5.7 mm,殉爆安全距离为8.8 mm。     

超临界CO2气爆煤体致裂机理实验研究

为提高超临界CO₂气爆低渗透煤层增透技术的应用水平,进一步研究超临界CO₂气爆煤体致裂机理,利用自主研发的超临界CO₂气爆装置,在多通道电液伺服相似材料试验台上,对原煤和混凝土大试件(1 m×1 m×0.5 m)进行了超临界CO₂气爆实验,用动态应变仪采集试件内部监测点处的变形和破坏信息,并用工业窥镜对爆破孔内裂隙分布进行了观测。分析气爆应力波的变化规律和气爆后试件的破坏形貌特征可知,距离气爆孔由近及远依次分为粉碎区、裂隙区和震动区,其形成机理为:超临界CO₂冲击气爆孔周围介质并形成远超介质抗压强度的球面纵波,介质在径向压应力作用下发生粉碎性破坏,形成粉碎区;应力波传播能量逐步衰减,不足以使介质产生压缩破坏,然而脆性材料抗压不抗拉,其产生的环向应力仍然使介质产生径向裂隙,应力波之后具有准静态加载作用的高压CO₂气体进入裂隙形成气楔,促使裂隙进一步发育和扩展,形成裂隙区;裂隙区以外的介质在低能量应力波的作用下只发生震动,未发生明显破坏,即震动区。裂隙的扩展速度与其到气爆孔距离符合“S”形曲线衰减,裂隙的高速扩展发生在粉碎区,低速扩展发生在裂隙区;距离气爆孔越远,测点的峰值应变越小,相同距离内节理裂隙等结构面越复杂,峰值应变减小的幅度越大且应变波形差别越大。