基于技术扩散的全社会能源效率空间条件收敛分析

我国各地区能源效率存在明显的差距,如何缩小地区能源效率差距成为了能源经济领域的热点问题.本文依据2000-2010年中国30省面板数据,运用空间误差条件β收敛模型分析了技术扩散对全社会能源效率收敛的影响,研究结果表明:①2000-2010年间,全社会能源效率呈现2000-2002、2002-2005和2005-2010的三阶段特征,经历上升、下降、再上升的变化过程,其中,2005-2010年提升速度最快,其经验值得借鉴;②全社会能源效率的绝对β收敛呈现由收敛至发散的三阶段变化过程;③全社会能源效率存在显著的空间滞后现象,其增长率的空间相依性不显著,但空间因素对全社会能源效率β收敛的正面影响有加强的趋势;④技术扩散从总体上使全社会能源效率的收敛速度提高1.8倍以上,且影响程度逐渐增强;⑤外商直接投资有助于提升全社会能源效率及其收敛速度;⑥不同时段的技术扩散对全社会能源效率的影响不同,且技术引进和国内技术市场技术流入对收敛的作用不显著.因此,引进外资是缩小地区间全社会能源效率差距的重要措施.     

MTBE装置潜在危险性分析及物料泄漏扩散后果模拟研究

MTBE装置处理的物料（混合C4、甲醇）具有易燃易爆性,若发生物料泄漏,将导致装置发生火灾爆炸。为了确保装置安全平稳、长周期运行,基于MTBE装置工艺技术特点,全面系统分析了装置的潜在危险性,总结出导致装置发生火灾爆炸事故的主要因素-物料泄漏;在此基础上,采用挪威DNV公司的SAFETI定量风险评价软件,建立混合C4、甲醇泄漏扩散模型,对物料泄漏导致的主要事故类型（喷射火、池火等）进行模拟,得出泄漏扩散引发火灾爆炸事故的危害范围。结果表明：该模拟研究能够反映出泄漏扩散过程和破坏范围,取得了较真实的事故影响范围曲线图,可以为设计人员更加详细了解MTBE装置发生事故的危害性及企业加强重点部位监控、制定防范措施、编制事故应急预案提供重要参考依据。     

Effects of significant damage of flame gap surfaces in flameproof electrical apparatus on flame gap efficiency

Electrical apparatus for use in the presence of explosive gas atmospheres has to be specially designed to prevent the apparatus from igniting the gas. Flameproof design is one of several options, and one requirement is then that any holes and slits in the enclosure wall be designed to prevent a possible gas explosion inside the enclosure from being transmitted to an explosive gas cloud outside it. Current standards (IEC) require that joint surfaces have a surface roughness of <6.3 μm. Any damaged joint surface has be restored to this quality. The present investigation has demonstrated that flame gap surfaces in flameproof electrical apparatuses can suffer considerable mechanical and corrosive damage before the flame gaps no longer function satisfactorily. In some cases very significant mechanical surface damage in fact improves the gap performance. This indicates that current high costs of repairing and replacing flameproof electrical apparatus in process plants offshore and onshore can be reduced considerably without any increase of the explosion risk.     

基于非恒定流的污染物迁移扩散随机模拟

针对目前大部分河流都受到不同程度污染的现状,研究了基于非恒定流的污染物迁移扩散随机模拟方法。通过一维非恒定流数值计算和流场模拟,得到了水库开闸放水后下游各个断面的水位、流量、流速等数据,并以此为基础,利用蒙特卡洛法对水库开闸放水前后下游典型断面的COD和NH3-N等进行污染物迁移扩散随机模拟,并将模型应用于文峪河下游。结果表明,文峪河水库开闸放水后,COD和NH3-N的污染带长度和宽度均有不同程度的减小,污染带向排污一侧岸边集中。研究成果可为解决河流污染现状与水库调度提供参考。     

填埋场内温度场下渗滤液饱和带内硫酸盐还原行为表征

填埋场内渗滤液饱和带是物质交换和生化反应的活跃区域,也是含硫恶臭的主要发生源.本研究探究了填埋场内温度场下渗滤液饱和带内硫酸盐还原行为特征,结果表明,在25～55℃逐步升温的温度场下,渗滤液饱和带内的硫酸盐还原行为逐步增强且差异显著.渗滤液饱和带纵向SO42-和DOC迁移转化规律各异但趋势相同.硫酸盐还原行为主要发生在固液交界区和固相区,且固液交界区的电子供、受体呈特定化学计量关系.电子供体是引起硫酸盐还原行为差异的主要原因.本研究揭示的温度场下渗滤液饱和带内硫酸盐还原行为可为填埋场精准除臭提供重要依据.     

丹江口水库氮磷内源释放对比

利用柱状沉积物采样器在丹江口水库采集不同点位原位柱状沉积物,通过静态培养释放实验及间隙水分子扩散模型两种方法获取沉积物-水界面N和P释放速率,分析水体N和P释放特征.结果表明,不同采样点N和P界面交换速率差异显著.静态培养条件下,5个点位NH_4~+-N和PO_4~(3-)-P释放速率分别为13. 07～24. 88 mg·(m~2·d)~(-1)和3. 06～6. 02 mg·(m~2·d)~(-1);分子扩散模型条件下,5个点位NH_4~+-N和PO_4~(3-)-P释放速率分别为2. 67～7. 25 mg·(m~2·d)~(-1)和0. 04～0. 18 mg·(m~2·d)~(-1). N和P释放速率总体呈北高南低的趋势,支流N和P最低释放速率分别是主库区最高释放速率的1. 48和1. 57倍.两种方法均表明郭家山支流N和P的释放速率最高,具有较大内源N和P释放风险.比较两种方法发现,利用Fick定律计算出的界面N和P释放速率明显小于柱样模拟方法得出的结果,N和P的R/F值分别为3. 43～4. 98和29. 67～72. 88,这表明用分子扩散模型法进行内源释放速率估算时,偏离真实情况较大,而原柱样静态模拟实验则较贴近真实情况.     

毛细管柱气相色谱法测定环境空气中1,2-二氯乙烷

采用毛细管柱气相色谱法测定环境空气中的1,2-二氯乙烷,用活性碳吸附,二硫化碳解析,FID检测器分析.方法在0 mg/L～311mg/L范围内线性良好,当采样体积为20 L时,最低检出质量浓度为0.006 mg/m3,标准溶液平行测定的RSD≤2.2%,加标回收率为98.4%～101%.     

A study on the obstacle-induced variation of the gas explosion characteristics

A study on the variation of the gas explosion characteristics caused by the built-in obstacles was conducted in enclosed/vented gas explosion vessels. It has been well known that the obstacles in pipes and long ducts would accelerate the flame propagation, and cause the transition from deflagration to detonation. In this study, the explosion characteristics and the flame behavior of vented explosions and constant-volume explosions were investigated. Experiments were carried out in a 270-liter and 36-liter hexahedron vessels filled with LPG–air mixture. The explosion characteristics of the gas mixture were determined by using a strain-responding pressure transducer. The flame behavior was recorded by using a high-speed video camera. The shape and the size of the obstacle, and the gas concentration, were adjusted in the experiments.

It can be seen from the experimental results that, instead of being accelerated, the flame propagation inside the explosion vessel is decelerated by the plate obstacles fixed at the bottom of the vessel. Also, the characteristics of the enclosed explosion are not so affected by the built-in obstacles as those of the vented explosion are. It is believed that the eddy-induced turbulence behind the obstacle decelerates the flame propagation.     

Transport of volatile compounds in porous media in the presence of a trapped gas phase

The presence of an immobile gaseous phase in an otherwise-saturated porous medium affects the transport of volatile compounds. The linear theory of partitioning tracers suggests that a volatile tracer introduced into such a system should be retarded with a constant retardation factor. Using high concentrations, however, the saturation of the gaseous phase will change as an effect of the tracer test itself. Competitive gas transfer among all volatile compounds and the change of saturation may lead to tracer concentrations that are temporarily higher than those injected. We analyze the system in the framework of the coherence theory by Helfferich [Soc. Pet. Eng. J. 21 (1) (1981) 51]. The governing equations are formulated as functions of total concentration, i.e., the mass of solutes in all phases per pore volume. Neglecting dispersion and mass-transfer kinetics, we derive the characteristic form of the resulting system of hyperbolic equations. In a system with N volatile compounds, a variation of the concentrations splits up into N waves, each traveling with its own characteristic velocity. If the presence of a gaseous phase is sustained, one wave will be a standing one. We perform numerical model calculations for tracers with various Henry's law coefficients and show that the results agree with the semi-analytical solution obtained by coherence theory.