压力容器无损检测 --长管拖车气瓶的无损检测技术

长管拖车是新类型的压力容器,作为一种高效运输工具,在许多领域应用广泛。综述了国内外拖车气瓶在制造和使用过程采用的各种无损检测方法及标准。方法包括超声、磁粉、渗透和声发射检测等。并介绍了各种无损检测方法的特点。     

水泥基复合材料微结构破坏声发射研究

研究不同组分的水泥基复合材料在三点弯曲负荷下,材料内部微结构破坏的声发射特性。结果表明,在加载初期声发射事件发展较为缓慢,且出现的主要是一些低振幅的声发射信号;而在峰值载荷附近,声发射事件数快速增长且开始有大量高振幅声发射信号出现。循环荷载作用下,粗集料水泥砂浆声发射呈现Felicit效应,而结构密实的活性粉末混凝土呈现Kaiser效应。     

Axial characterization of catalytic activity in close-coupled lightoff and underfloor catalytic converters

A exhaust system consisting of a close-coupled Pd technology 32 in³ lightoff converter and Pt/Rh technology 170 in³ underfloor converter was vehicle-aged for 56000 miles on a vehicle equipped with a 3.8 l engine. Following this aging, the converters were taken off the vehicle and cut into 1″ thick sections along their axis and characterized for lightoff and warmed-up activity using a laboratory reactor to simulate vehicle exhaust. Each section was also analyzed for the quantity of oil additive poisons (phosphorus and zinc) deposited. Following this initial characterization, the phosphorus and zinc deposits were removed, and the sections were characterized again for lightoff and warmed-up activity. This procedure was used to qualitatively determine the relative contribution of oil additive poisoning and thermal sintering to the total activity deterioration as a function of axial position in the catalyst monoliths.

Analysis of the lightoff converter as taken from the vehicle showed a dramatic axial gradient in the lean and stoichiometric lightoff and warmed-up (600°C) performance for HC, CO and NO_x, with most of the deterioration having taken place in the forward-most 1″ section of the converter, which was consistent with the gradient in the deposition of phosphorus (P) and zinc (Zn) in this converter. Comparison of these data sets with those obtained after removal of the P and Zn poisons indicates that most of the total deterioration of lean HC and CO activity can be attributed to P and Zn poisoning of the forwardmost 1″ section. When tested under stoichiometric conditions, most of the deterioration of HC activity is attributable to P and Zn poisoning, while most of the deterioration of CO and NO_x activity is attributable to thermal deterioration. A similar activity and poison deposition gradient was detected in the underfloor converter, but to a smaller extent.     

铬盐清洁生产中铬渣的综合利用

利用二氧化碳与液相氧化铬盐清洁生产工艺所产生的铬渣反应 ,得到碳酸氢镁溶液和富铁渣。碳酸氢镁溶液经加热分解得到轻质碳酸镁产品 ,富铁渣可以作为水泥行业原料铁精矿的替代品 ,最终实现了铬铁矿资源的充分利用和铬盐生产的零排放。     

Scientific basis for establishing country greenhouse gas estimates for rice-based agriculture: An Indian case study

A comprehensive scientific assessment of CH₄ budget estimation for Indian rice paddies, based on a decade of measurements in India, is presented. Indian paddy cultivation areas contain soils that have low to medium levels of soil organic carbon. The average seasonally integrated CH₄ flux (E _sif) values calculated from these measurements were 15.3 ± 2.6 g m^–2 for continuously flooded (CF), 6.9 ± 4.3 g m^–2 for intermittently flooded (IF) single aeration (SA) and 2.2 ± 1.5 g m^–2 for IF multiple aeration (MA) rice ecosystems. For CF and IF (MA) rice ecosystems having high soil organic carbon, without organic amendments, the CH₄ flux (E _sif) may be increased by 1.7 times relative to low soil organic carbon, whereas it may enhance by 5.3 for CF if amended organically. Organic amendment and high soil organic carbon paddy areas do not alter the methane budget estimates for India (3.6±1.4 TgY^–1) much, due to their small paddy harvested area. Methane estimated using average emission factors (E _sif) for all paddy water regimes, which include harvested areas having soils with high organic carbon and organic amendments, may give a budget of 5 TgY^–1 for India.     

基于超高温光谱的C/C材料烧蚀产物研究

用“星形”等离子发生器及国产的等离子体火炬进行了炭基复合材料烧蚀实验，采用实验中光谱检测对烧蚀产物进行了分析。经分析发现：在“星形”等离子发生器产生的3500K以下烧蚀环境的光谱中，产物以CO为主，而在国产的等离子体火炬产生的5500K以上烧蚀环境的光谱中，产物以CN、C2、C1和CO为主。光谱检测结果与热化学烧蚀计算的产物吻合得很好，验证了热化学计算的正确性。     

In-situ studies of electron field emission of single carbon nanotubes inside the TEM

Electron field emission characteristics of individual multi-walled carbon nanotubes (MWCNTs) were investigated in situ inside the transmission electron microscope (TEM). For a single MWCNT it was found that while field-emission can hardly occur from the side of the nanotube, a curved nanotube may result in finite side emission and the best emission geometry is the top emission geometry. Current-voltage (I-V) measurements made at different vacuum conditions and voltage sweeps emphasize the importance of the adsorbates on the electron field emission of MWCNTs. For a contaminated MWCNT, although the field emission current was reduced, the stability of its emission was improved. A current of up to several tens of μA was observed for a single MWCNT, but it was found that long time emission usually results in drastic structure damage that may lead to sudden emission failure.     

三轴应力下盐岩声发射特征研究（研究生论坛稿件）

利用MTS815 Flex Test GT岩石力学试验系统和PCI–2声发射(AE)三维定位实时监测系统,开展不同围压下盐岩的三轴压缩声发射定位试验,探讨盐岩轴向加载过程中声发射特征的围压效应。研究结果表明：盐岩AE定位点多少与振铃计数率大小、能率高低具有良好的一致性。声发射高计数、高能率、定位点集聚段等随围压增加而滞后。低围压下,盐岩发生剪切破坏,高计数、高能率、AE定位点集聚段主要出现在屈服阶段和峰值应力前阶段;高围压下,盐岩呈塑性大变形特征,高计数、高能率、AE定位点集聚段主要在峰值阶段及峰后阶段出现。围压增加,累计计数和定位点的总量呈减少趋势;最大能率和累计能量随围压增加而减小,5MPa约分别为30MPa的43倍和22倍。     

UHMWPE/LDPE复合材料拉伸破坏的声发射特性研究(Ⅱ)

本文续“UHMWPE/LDPE复合材料拉伸破坏的声发射特性研究(Ⅰ)”,进一步研究了UHMWPE/LDPE复合材料拉伸破坏的声发射特性,具体研究了[0°]、[90°]在拉伸破坏过程中声发射参数特征,并对拉伸破坏机理进行了初步的研究。     

Whispering gallery modes in photoluminescence and Raman spectra of a spherical microcavity with CdTe quantum dots: anti-Stokes emission and interference effects

We have studied the photoluminescence and Raman spectra of a system consisting of a polystyrene latex microsphere coated by CdTe colloidal quantum dots. The cavity-induced enhancement of the Raman scattering allows the observation of Raman spectra from only a monolayer of CdTe quantum dots. Periodic structure with very narrow peaks in the photoluminescence spectra of a single microsphere was detected both in the Stokes and anti-Stokes spectral regions, arising from the coupling between the emission of quantum dots and spherical cavity modes.