烟气湍流效应对火灾图像探测的影响

烟气是火灾过程的重要物理现象,烟气的湍流效应是火灾图像探测的重要影响因素,分析了烟气湍流反应对火灾图像探测的影响,得出了一些烟气湍流效应的图像特征,为多参数特征的火灾探测提供了理论依据。     

火电厂烟气抬升的积分模型研究

根据流体力学的基本方程,考虑引起烟气抬升不同阶段的掺混原因,将产生的掺混率叠加导出一个简单的掺混函数,从而得到一个计算烟气抬升运动的积分模型,并与试验结果进行了比较。     

普光高含硫气田集输管道冲蚀规律及预测模型研究

基于灰色关联分析方法,根据集输管道在线腐蚀监测数据,采用剪切应力表征湍流两相流动对管道内壁的冲刷作用,以湍流强度表征湍流传质强化对腐蚀的影响程度,同时集成普光气田集输管道室内静态腐蚀实验数据,建立了普光气田集输管道动态腐蚀预测模型,为普光气田集输系统腐蚀监测及安全管理提供了依据。     

紊流作用下泥沙释放磷的试验及数值模拟

为研究水体紊动对泥沙释放污染物的影响,引入近似均匀紊流模拟装置,开展不同强度紊动作用下泥沙运动释放磷动态过程及基本规律的试验,研究表明:紊动扩散作用对泥沙解吸释放磷有着十分重要的影响,紊动较弱时,泥沙尚未起动,床面泥沙颗粒吸附的磷元素解吸至孔隙水中,在垂向紊动扩散作用下输送至上覆水中,将使得上覆水中溶解态磷浓度增大;紊动作用较强时,泥沙逐渐悬扬至水体中,悬浮泥沙颗粒吸附的磷元素直接解吸至上覆水中,泥沙浓度越高,溶解态磷含量增长速率越大,达到平衡的时间越短.通过耦合紊流模型、水流泥沙数学模型、污染物对流扩散模型和Langmuir吸附动力学方程建立了紊动作用下泥沙释放磷的垂向一维数学模型,针对试验条件进行数值模拟,模拟结果与试验数据吻合较好,平均相对误差低于10%,可为模拟天然水体中泥沙悬浮释放磷的时空演化提供参考.     

梯形巷道平均风速分布特征的数值与实验研究

为实现矿井巷道内风量的准确监测,基于3D数值模型,对梯形截面巷道内平均风速的分布规律进行了数值分析,并通过实验研究对模拟结果进行对比验证,同时在不同断面尺寸及不同通风风速条件下,数值分析了梯形巷道内紊流充分发展截面上平均风速点的分布特征。结果表明:平均风速分布呈现环状连续分布,数值结果与实验结果符合良好;梯形截面上平均风速点的分布与通风风速无关,仅与巷道截面特征和参数有关;得到了梯形截面平均风速分布曲线在巷道顶部的特征方程。     

马兰黄土对铜的吸持及其形态变化的影响

采用谐振式紊动模拟装置,模拟了均匀紊动条件下马兰黄土与铜的相互作用及其垂向浓度分布,测定了铜的形态和含量,并用模型ＭＩＮＴＥＱＡ２对平衡形态进行计算分析,投沙量(Ｓ０)范围为５－８００ｋｇ·ｍ３．结果表明,黄土吸持铜的量和水相铜浓度均随投沙量的增加而快速下降．在投沙量１００－２００ｋｇ·ｍ３处,固液两相铜的浓度发生突变．黄土上的铜以碳酸盐结合态为主,达９２%以上,表明铜的吸持过程可能以沉淀为主．模型计算结果进一步证实,无论是高浓度还是低浓度泥沙,黄土吸持铜的过程主要以沉淀为主,但高浓度和低浓度的沉淀组成及其比例不同,Ｓ０＜１００ｋｇ·ｍ３时为Ｃｕ４(ＯＨ)６ＳＯ４,Ｓ０＞１００ｋｇ·ｍ３时为Ｃｕ２(ＯＨ)２ＣＯ３．实验分析和模型计算都表明,由于马兰黄土富含１０%以上的碳酸钙而使体系的ｐＨ值升高,高浓度泥沙因此具有更强的以沉淀为主的吸持铜的能力。     

基于ATG实报的空中颠簸预防管理系统设计

在对颠簸伤害事件原因分析的基础上,设计了基于ATG实报的空中颠簸预防管理系统,该系统设计主要包括:开发QAR计算EDR程序,通过EDR指标提高颠簸预报精度;开发颠簸管理平台,实现颠簸信息的有效传递;利用ATG技术使颠簸预报向颠簸实报提升,提高颠簸信息的实时性。该解决方案可实现空地高精度颠簸风险实时自动预警,有效降低颠簸伤害。     

Turbulent Ventilation of a Street Canyon

A selection of turbulence data corresponding to 185 days of field measurements has been analysed. The non-ideal building geometry influenced the circulation patterns in the street canyon and the largest average vertical velocities were observed in the wake of an unbroken line of buildings. The standard deviation of vertical velocity fluctuations normalised by the ambient wind speed was relatively insensitive to ambient wind direction and sensor position, and it was usually larger than the corresponding 1-hour average velocity. Cross-correlations of spatially separated velocity measurements were small, and this suggests that most of the velocity fluctuations were fairly local and not caused by unsteady street vortices. The observed velocities scaled with the ambient wind speed except under low-wind conditions.     

湍流状态下甲烷爆炸特性的实验研究

利用20L近球形气体爆炸反应装置,测试甲烷在宏观静止和湍流两种不同状态下的爆炸特性。实验结果表明:甲烷的爆炸极限受其流动状态的影响不明显;湍流状态下甲烷爆炸压力Pm和爆炸压力上升速率(dp/dt)m较宏观静止状态明显增大,爆炸压力峰值时间tm明显缩短,其中爆炸压力上升速率受湍流影响较为显著;甲烷浓度不同,其爆炸受湍流影响的程度也不同,较高浓度(11%～16%)时的Pm受湍流的影响程度较大,越靠近最佳浓度(dp/dt)m和tm受湍流的影响程度越大;同一浓度下Pm和(dp/dt)m随着湍流的加强而增大,tm则缩短。该研究表明,避免和减少湍流对矿井瓦斯爆炸过程的抑制具有重要作用。     

Experimental investigation of the effect of sediment transport patterns on the adsorption of cadmium ions onto sediment particles

The mechanism of flow turbulence, sediment supply conditions, and sediment transport patterns that affect the adsorption of cadmium ions onto sediment particles in natural waters are experimentally simulated and studied in this study both in batch reactors and in a turbulence simulation tank. By changing the agitation conditions, the sediment transport in batch reactors can be categorized into bottom sediment-dominated sediment and suspended sediment-dominated sediment. It is found that the adsorption rate of bottom sediment is much less than that of suspended sediment, but the sediment transport pattern does not affect the final (equilibrium) concentration of dissolved cadmium. This result indicates that the parameters of an adsorption isotherm are the same regardless of the sediment transport pattern. In the turbulence simulation tank, the turbulence is generated by harmonic grid-stirred motions, and the turbulence intensity is quantified in terms of eddy diffusivity, which is equal to 9.84F(F is the harmonic vibration frequency) and is comparable to natural surface water conditions.When the turbulence intensity of flow is low and sediment particles stay as bottom sediment, the adsorption rate is significantly low, and the adsorption quantity compared with that of suspended sediment is negligible in the 6 h duration of the experiment. This result greatly favors the simplification of the numerical modeling of heavy metal pollutant transformation in natural rivers. When the turbulence intensity is high but bottom sediment persists, the rate and extent of descent of the dissolved cadmium concentration in the tank noticeably increase, and the time that is required to reach adsorption equilibrium also increases considerably due to the continuous exchange that occurs between the suspended sediment and the bottom sediment.A comparison of the results of the experiments in the batch reactor and those in the turbulence simulation tank reveals that the adsorption ability of the sediment, and in particular the adsorption rate, is greatly over-estimated in the batch reactor.