Electrospun nanofiber composites with micro-/nano-particles for thermal insulation

Polyacrylonitrile (PAN) nanofiber and silica aerogel (SAG) laminated composites were prepared via electrospinning for thermal insulation. Conventional single nozzle and co-axial electrospinning were used to increase the fraction of aerogel particles in the composite sheets while maintaining the mechanical strength of the sheet. When the core-shell electrospinning technique with co-axial nozzle was applied, the proportion of aerogel particles increased two fold without a deterioration of the mechanical properties. The average thermal conductivity of the laminated composite sheet was reduced by approximately 12.5% as compared to the nanofiber composite prepared using the single-nozzle electrospinning technique. For additional reduction in thermal conductivity, hollow glass microspheres (HGM) was inserted between the interlayer spacing of the electrospun sheets to increase the interlayer spacing. When HGM particles were inserted, it was observed that the thermal conductivity decreased by approximately 20% compared to that of the specimen without particles.     

单片集成电吸收调制分布反馈激光器

提出一种选择区域外延双有源区叠层(SAG-DSAL)结构新技术,基于此技术设计研制了单片集成电吸收调制激光器(EML),SAG-DSAL-EML管芯的阈值电流为20mA,工作电流为100mA时的出光功率为10mw,由吸收调制器(EAM)加-3V偏压时的消光比为12dB,实现了简化制作工艺并提高器件性能的预期目的,有望用...     

落重试验在碎磨工艺设计与优化中的应用

落重试验作为一种用于自磨(半自磨)机选型计算的矿石试验方法近些年来在国内得到越来越多的应用。简要介绍这种与粉碎数学模型密切相关的试验方法、物料特性参数及其在碎磨工艺设计与优化上的应用。     

Acoustic emissions simulation of tumbling mills using charge dynamics

Knowledge of the internal variables of a mill is of importance in design and performance optimization of the mill, notwithstanding the difficulty in measuring these variables within the harsh mill environment. To overcome this problem, the research has focused on measuring the internal parameters through non-invasive measurement methods such as the use of the vibration/acoustic signal obtained from the mill. Alternatively, virtual instruments, such as discrete element methods (DEM), are employed. Here, a methodology is developed to simulate on-the-shell acoustic signal emitted from tumbling mills using the information extracted from a DEM simulator. The transfer function which links the forces exerted on the internal surface of the mill and the acoustic signal measured on the outer surface is measured experimentally. Given this transfer function and the force distribution obtained from the DEM simulation, and assuming a linear time-invariant response, the on-the-shell acoustic of a laboratory scale ball mill has been simulated. Comparison of this simulated signal with the signal measured experimentally can be used as a criterion to judge the validity of the DEM simulations, and as a tool for enhancing our understanding of both DEM simulations and the use of acoustics within the context of mineral processing. The results derived from preliminary experiments on a laboratory scale mill shows satisfactory agreement between the actual measurement and the simulated acoustic signal.     

选择外延MOCVD研制DFB激光器和模斑转换器集成器件

研究了利用选择外延生长的InGaAsP材料的厚度增强因子和带隙波长的性质,最大的厚度增强因子为2.9.利用选择外延技术研制的DFB激光器和模斑转换器的集成器件,阈值为10.8mA-在60mA下输出功率为10mW,边模抑制比为35.8dB,垂直方向上的远场发散角从34°减少到9°,垂直方向上的1dB偏调容差为3.4μm.     

水平井蒸汽辅助重力驱数学模型的建立及求解方法

油藏与水平井段耦合的蒸汽辅助重力驱数学模型及其求解方法已经建立。本文在此基础上考虑建立沿水平井井筒方向上有质量、能量损失的一维多相管流数学模型。如果能研制相应的油藏模拟软件,可预测水平井蒸汽辅助重力驱蒸汽腔室的大小及形状的动态变化,模拟计算毛管力、蒸汽干度、地层深度等对蒸汽腔室发育程度的影响。     

多源矿点配矿的SAB流程磨矿优化控制技术应用

选矿生产管理过程自动化、信息化与智能化的融合技术,已经成为进一步优化选矿厂资源配置,全面提升选矿厂安全生产、经营管理科学化、现代化水平的有效手段。以某选厂典型的SAB流程为例,介绍了一套优化控制系统在多源矿点配矿磨矿分级流程中的应用方法和使用效果。在目标流程中通过采用智能给料、专家系统、模糊控制和参数自适应等先进的检测和过程控制技术实现了磨矿生产流程的智能控制。     

物料粒径对半自磨机衬板磨损的影响

采用数值计算方法分析粒径对半自磨（SAG）机衬板磨损的影响。采用离散单元法（DEM）描述物料运动,采用切向碰撞能量磨损模型（SIEM）预测壁面磨损. 结果表明,粒径大小对衬板磨损存在显著影响. 粒径增大,衬板磨损亦随之增大;当粒径较小时（如：d=30 mm）,磨损增幅尤为明显. 提升条的磨损主要在经过底脚区与颗粒发生剧烈碰撞时产生,不同粒径大小下均如此. 大颗粒获得的动能要远远大于小颗粒,且相比于小颗粒,大颗粒改变运动状态需要更长的时间,导致剧烈磨损的持续时间亦明显增加. 粒径大小对磨损在提升条上的分布无明显影响.     

选择外延MOCVD研制DFB激光器和模斑转换器集成器件

研究了利用选择外延生长的InGaAsP材料的厚度增强因子和带隙波长的性质,最大的厚度增强因子为2.9.利用选择外延技术研制的DFB激光器和模斑转换器的集成器件,阈值为10.8mA-在60mA下输出功率为10mW,边模抑制比为35.8dB,垂直方向上的远场发散角从34°减少到9°,垂直方向上的1dB偏调容差为3.4μm.