光度计式烟尘浓度监测仪的标定

在过滤式测尘仪前连接一测烟管,即能利用锅炉烟尘对光度计式烟尘浓度监测仪进行标定,此标定值表征仪器光束所穿过烟道上各处烟尘的平均浓度与测定量的比例系数。     

燃煤烟气除尘系统技术经济评价方法

主要介绍燃煤烟气除尘技术在总量控制中的应用。通过对燃煤烟气除尘系统技术经济指标体系以及技术经济分析、评价方法的确定,为筛选各种燃煤烟尘控制技术提供统一的技术经济分析和评价方法。      

上海内环高架沿线灰尘重金属污染分析与评价

对上海市内环高架沿线街道灰尘重金属污染进行了调查,结果表明,与道路交通因素相关的重金属Pb、Cd、Cu和Zn均具有较高的含量水平,分别为上海市土壤背景值的9.3倍,7.5倍,9.0倍和8.8倍。除了重金属Hg以外,其他7种重金属平均含量均表现为浦西段高于浦东段,说明内环高架浦西段相对于浦东段具有较高的重金属积累。而污染指数评价的结果也表明了上述4种重金属的污染程度超过了其他重金属,已经达到了中度污染水平。     

A comparative study between two ignition sources: Electric igniter versus pyrotechnic igniter

The risk assessment of combustible explosive dust is based on the determination of the probability of dust dispersion, the identification of potential ignition sources and the evaluation of explosion severity. It is achieved in most of cases with the two main experimental normalized devices such as the Hartmann tube (spark ignition) and the 20 L spherical bomb (with two 5 kJ pyrotechnic ignitors).Ignition energy of the 5 kJ ignitor is well calibrated and generates a reproducible ignition. But, on the other hand, this ignition is not punctual and the over pressure produced is nearly 2 bar. Moreover, the pyrotechnic igniter accelerates the combustion with multi ignition points in a large volume and that disturbs the flame propagation. In this way, this ignition source does not allow to analyze the combustion products because the composition of the pyrotechnic igniter was found in the combustion products.This paper deals with the comparison of two ignition sources in the 20 L spherical bomb. Different explosive dusts of great industrial interest are studied with electrical and pyrotechnic ignitors, in order to understand, first, the influence of each type of igniter on the explosion behaviour and then to evaluate the possibility of establishing a correspondence between parameters obtained with these two ignition sources.Severity parameters of nicotinic acid, aluminium powder and titanium alloy were measured by using the two types of ignition system in our 20 L spherical bomb equipped with the Kühner dihedral injector. The explosion overpressure $\mathrm{P}$ and the rate of pressure rise $\left(\raisebox{1ex}{$dP$}\!\left/ \!\raisebox{-1ex}{$dt$}\right.\right)$ were measured in a large range of concentration allowing to propose correlations between electrical and pyrotechnic ignition for each parameter and each type of powder. These correlations aim to link the tests used with two different collections of experimental parameters for the same dust. The relevance of these correlations will be discussed.     

室内尘埃中铅的赋存形态与儿童血铅的相关性研究

有关室内尘埃中铅的赋存形态与儿童血铅的相关性研究尚未见报道。在对某地儿童血铅进行调查期间,发现当地儿童血铅浓度与室内尘埃中铅的水溶态、离子交换态、腐殖酸结合态、铁锰氧化态、强有机结合态和残渣态呈正相关,但不显著,无统计学意义。但与总铅浓度呈显著正相关(R=0.447,P=0.032),与铅的碳酸盐结合态呈高显著相关(R=0.537,P=0.008)。在此基础上,将儿童血铅分别与尘埃中铅暴露量、摄入量和潜在剂量进行相关分析,结果表明,儿童血铅与室内尘总铅摄入量和总铅潜在剂量正相关但无统计意义,与尘总铅暴露量显著相关(R=0.431,P=0.040),与碳酸盐态的暴露量(R=0.537,P=0.008)、摄入量(R=0.538,P=0.008)和潜在剂量(R=0.540,P=0.008)高度显著相关。提示在土壤和尘埃中铅的碳酸盐态含量较高的地区,碳酸盐态铅可能是造成儿童血铅超标的主要原因。     

Dust cloud evolution and flame propagation of organic dust deflagration under low wall influence

The present study discusses experiments on organic dust explosions in a setup with low wall influence. The proposed apparatus decouples the dust dispersion and the deflagration event in two separate compartments. The use of a continuous-wave laser to illuminate the centre plane of the observation chamber allows capturing both, the dust cloud and the flame during the same experiment and eliminates typical problems caused by the limited dynamic range of high-speed cameras. A k-means clustering method is used for image segmentation to obtain the spatial extent and the propagation velocities of the unreacted particle cloud and the flame zone. Spatially resolved velocities are calculated by the additional use of an optical flow method. The main goal of the presented setup and image processing method is to provide high quality validation data for the development of numerical models on dust deflagration.     

The simulation of long-range transport of ¹³⁷Cs from East Asia to Japan in 2002 and 2006

To evaluate the quantities of ¹³⁷Cs from past nuclear tests being transported to and deposited in Japan by naturally-occurring phenomena, the authors developed long-range transport models for ¹³⁷Cs considering Asian dust. The simulation using these models backed the observed recent increase of ¹³⁷Cs deposition along the coast of the Sea of Japan in early spring. For the sake of public safety, it is vital to ascertain whether an increase of radioactive deposition is caused by natural phenomena or a nuclear accident. The observations in recent years have suggested that dust and soil containing ¹³⁷Cs is transported from the regions around Inner Mongolia to Japan by the wind. In this paper, using observation data from the early spring of 2002 and 2006, the authors have found good agreement between the simulations and the measurements. The simulations reproduced the entrainment of ¹³⁷Cs and subsequent transport to Japan caused by strong winds associated with low pressure areas around the Inner Mongolian grasslands. The most likely cause of high-level ¹³⁷Cs deposition over northern Japan during March 2002 was ¹³⁷Cs associated with particles transported at low-altitude (1 km) and subjected to precipitation on the 22nd to 24th.     

A numerical model for the prediction of the minimum ignition temperature of dust clouds

This paper presents a numerical model for the prediction of the minimum ignition temperature (MIT) of dust clouds. First, a physical model is developed for the dust cloud ignition in the Godbert-Greenwald furnace. A numerical approach is then applied for the MIT prediction based on the physical model. The model considers heat transfer between the air and dust particles, the dust particle reaction kinetics, and the residence times of dust clouds in the furnace. In general, for the 13 dusts studied, the calculated MIT data are in agreement with the experimental values. There is also great accordance between the experimental and numerical MIT variation trends against particle size. Two different ignition modes are discovered. The first one consists in ignition near the furnace wall for bigger particles characterized by rather short residence times. In the second mode, the ignition starts from the center of the furnace by self-heating of the dust cloud for smaller particles with longer residence times. For magnesium, as dust concentration increases, the lowest ignition temperature of the dust cloud IT(conc) decreases first, then transits to increase at a certain point. The transition happens at different dust concentrations for different particle sizes. Moreover, the MIT of the magnesium dust cloud generally increases as particle size increases, but the increasing trend stagnates within a certain medium particle size range.