Environmental dispersivity in free-water-surface-effect dominated wetland: multi-scale analysis

Distinct from the case with width-dominated shallow wetland flows, the longitudinal evolution of contaminant concentration in the most-typical pattern of wetland as dominated by free-water-surface-effect is characterized by a multi-scale analysis in the present study. An environmental dispersion model for the evolution of the mean concentration is deduced as an extension of Taylor's classical formulation by Mei’s multi-scale analysis. Corresponding environmental dispersivity is found identical to that determined by the method of concentration moments.     

改进的产业碳关联系数及应用 ——以上海为例

投入产出分析中重要的影响力系数和感应度系数被引入到我国的产业环境关联研究中,但采用的计算方法却多是存在缺陷的传统公式,对指标的政策意义解读也有待深入.在梳理2项指标前沿发展的基础上,以部门最终产品构成系数为权数,改进了表征产业碳关联的碳影响力系数和碳影响诱导系数(代替原碳感应度系数)的计算公式,并指出前者主要对应产业政策,对部门划分水平较不敏感,而后者主要对应节能减排政策,对部门划分水平较敏感.将改进的指标应用于2010年上海市,结果表明,其产业政策应扶植服务业和先进制造业,鼓励重化工业和专用设备制造业转型,逐步淘汰多数传统中低端制造业,节能减排政策的重点实施部门则应扩大到部分高能耗服务业.     

铬污染土壤超低频复电阻率频散特性

在超低频段(2-5~26Hz)内,研究了铬污染土壤复电阻率在不同含水率、铬含量和孔隙率下的幅值及相位频散特性. 结果显示,铬污染土壤复电阻率的幅值随频率的增大呈单调递减趋势,但相位随频率的变化曲线呈平放的S形. 含水率、铬含量和孔隙率的变化均会引起土壤复电阻率的幅值和相位大小的改变,而相位峰值的位置只对含水率及孔隙率的变化较为敏感,与铬含量变化的关系不大. 含水率从0.08增至0.24时可导致相位峰值的位置产生约8Hz的右移;而当w(Cr6+)从0.5g/kg增至4.0g/kg时,相位峰值的位置基本不发生变化. 表明铬含量和含水率的增大均会引起电阻率减小的异常现象,若单纯地使用电阻率很难区分引起这2种异常现象的原因,但结合土壤复电阻率频散特性特别是相位峰值的位置可以进行有效判别,进而可判定铬污染场地的铬含量分布.      

十一镍锆钼杂多酸盐的合成、表征及超声强化降解染料废水

采用水溶液合成法制备了具有Keggin型结构的十一镍锆钼杂多酸盐Na6[Ni（Mo11ZrO39）].20H2O（NiZrMo）,并对其进行表征及分析.元素分析表明,镍锆钼之间的物质的量之比满足1∶1∶11的关系;热重/差热分析说明合成的杂多酸盐具有比较好的热稳定性并带有20个结晶水;红外光谱、X射线衍射及紫外光谱表征充分表明合成的杂多酸盐其阴离子仍保持Keggin型结构;扫描电镜分析表明,具有比较好的大分子化合物的基本特征和比较规则的晶体结构.以NiZrMo杂多酸盐为催化剂降解酸性绿B（AGB）染料废水,降解率最高可达95.72%.     

高架桥对街道峡谷内大气颗粒物输运的影响

随着我国城市汽车保有量的迅速攀升,城市中心区域的空气质量与生态环境急剧恶化.利用计算流体力学(CFD)数值模拟,研究了3种H/W(街道建筑物高度/峡谷宽度)下高架桥对街道峡谷内颗粒物扩散的影响.建立了街道峡谷内机动车尾气中颗粒物扩散模型,并给出了边界条件.采用标准k-ε模型与离散相模型对街道峡谷内部气流运动、颗粒物扩散及浓度分布进行了模拟计算,并计算了高架桥对风场及颗粒物扩散的影响.结果表明:H/W越大,街道峡谷内颗粒物浓度越高,同时颗粒物平均滞留时间越长.相对于没有高架桥的街道峡谷,高架桥附近区域风场变化明显,但对建筑物墙壁、地面及峡谷顶层处影响较小.街道峡谷内存在高架桥时,在墙壁较低处颗粒物浓度增加.      

猪粪中典型类固醇雌激素的固相萃取/GC-MS检测

以猪粪中常见且具有较大潜在危害的E1(雌酮),17α-E2(17α-雌二醇),17β-E2(17β-雌二醇)和E3(雌三醇)为研究对象,建立了猪粪中这4种典型类固醇雌激素的GC-MS(气相色谱-质谱)分析检测方法.着重优化了样品的前处理方法,包括对超声提取剂、超声提取时间、固相萃取淋洗剂、衍生化温度和时间的优化选择.结果表明:在优化的试验条件下,猪粪中的典型雌激素E1,17α-E2,17β-E2和E3检出限分别为8.0,2.5,5.1和3.3 μg/kg,平均加标回收率在92.3%～137.4%之间.      

非离子表面活性剂淋洗萘污染土壤的修复研究

采用土柱实验研究了非离子表面活性剂对焦化厂萘污染砂土的淋洗效果,同时研究了超声预处理对非离子表面活性剂土壤淋洗的增强效果及粉土和粘土对非离子表面活性剂土壤淋洗的不利影响.研究表明,1)1g·L-1的TritonX-100、AEO-9和Tween80对同一萘浓度(192.4mg·kg-1)的土壤洗脱效率分别为73.0%、81.5%和59.0%,2g·L-1的表面活性剂的洗脱效率要高于1g·L-1的洗脱率,分别为96.5%、95.1%和88.2%.2)对土壤进行短时超声处理(80Hz)促进了洗脱率的提高,超声10min的淋洗效果要高于超声5min的淋洗效果;土壤分别经5min和10min超声处理后,2g·L-1浓度的TritonX-100对萘的洗脱率从94%分别提高到98.8%和99.6%,洗脱时间从255min分别减少到172min和160min.3)砂土中含有粉土和粘土对洗脱效果有不利影响,且粘土的影响要更严重,当萘污染的砂土混入5%的粘土时,2g·L-1浓度的TritonX-100对萘的洗脱率从94.7%下降至73.8%,洗脱时间从255min增加至605min,而混入20%的粉土洗脱率仅下降到88.4%,洗脱时间增加至512min.     

Simulating mesoscale transport and diffusion of radioactive noble gases using the Lagrangian particle dispersion model

In order to simulate the impact of mesoscale wind fields and to assess potential capability of atmospheric Lagrangian particle dispersion model (LPDM) as an emergency response model for the decision supports, two different simulations of LPDM with the mesoscale prognostic model MM5 (Mesoscale Model ver. 5) were driven. The first simulation of radioactive noble gas ((85)Kr exponent) emitted during JCO accident occurred from 30 September to 3 October 1999 at Tokai, Japan showed that the first arriving short pulse was found in Tsukuba located at 60km away from the accidental area. However, the released radioactive noble gas was transported back to the origin site about 2 days later due to the mesoscale meteorological wind circulation, enhancing the levels of (85)Kr with the secondary peak in Tsukuba. The second simulation of atmospheric dilution factors (the ratio of concentration to the emission rate, chi/Q), during the underground nuclear test (UNT) performed by North Korea showed that high chi/Q moved to the eastward and extended toward southward in accordance with the mesoscale atmospheric circulations generated by mesoscale prognostic model MM5. In comparison with the measurements, the simulated horizontal distribution patterns of (85)Kr during the JCO are well accord with that of observation in Tsukuba such as the existence of secondary peak which is associated with the mesoscale circulations. However, the simulated level of (85)Kr anomaly was found to be significantly lower than the observations, and some interpretations on these discrepancies were described. Applications of LPDM to two mesoscale emergency response dispersion cases suggest the potential capability of LPDM to be used as a decision support model provided accurate emission rate of accident in case of a large accident.     

Evaporating liquid flow in a channel (An integral model based on shallow water flow approximation)

Liquefied Natural Gas (LNG) storage facilities generally include channels to convey potential spills of the liquid to an impoundment. There is increasing concern that dispersion of vapors generated by flow of LNG in a channel may lead to higher than limit vapor concentrations for safety at site boundary from channels that may be close to the dike walls. This issue is of recent concern to regulatory agencies, because the calculation of vapor hazard distance(s) from LNG flow in a channel is not required under existing LNG facility siting standards or regulations.An important parameter that directly affects the calculated LNG vapor dispersion distance is the source strength (i.e., the rate of vaporization of LNG flow from the wetted channel surfaces, as a function of spatial position and time). In this paper a model is presented which considers the variation of the depth of the flowing LNG with spatial location and time, and calculates the spatial and temporal dependence of the mass rate of vapor generation. Self similar profiles for the spatial variation of the thermal boundary layer in the liquid wetted wall and liquid depth variation are assumed. The variation with time of the location of the liquid spread front and the evaporation rate are calculated for the case of a constant LNG spill rate into a rectangular channel. The effects of two different channel slopes are evaluated. Details of the results and their impact on dispersion distances are discussed.     

Dispersion of the vapour cloud in the Buncefield Incident

Dispersion of the flammable vapour cloud in the 2005 Buncefield Incident is examined. Footage from security cameras around the site is analysed and the results from Computational Fluid Dynamics (CFD) simulations of the vapour dispersion are presented. It is shown that the shape of the terrain and the presence of obstacles significantly affected the dispersion of vapour from the overflowing tank. The CFD model is shown to produce similar qualitative behaviour to that observed in the incident, both in terms of the arrival time of the vapour cloud and its final depth.