共查询到18条相似文献,搜索用时 800 毫秒
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各种热电、核电厂排出的热污(废)水在直接进入环境流体之前,以多孔口浮射流的形式释放污水并确保污水在排污口快速混合非常重要。精确的了解和预测多孔浮射流的特性与混合状况有很重要的意义。针对同向流动环境中多圆形孔口热水排放的情况,采用雷诺应力模型进行数值模拟,得到了不同流速比和不同射流温度下的流场和温度场、浮射流的轨迹线、轴线上温度和速度的衰减规律,并且分析了不同孔间距、流速比和射流温度对流场中流速和温度的影响。 相似文献
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在清水实验中研究了中试气升式氧化沟单侧廊道流速分布及进气量对升流区和直段流速的影响.中试装置容积54m3,当进气量按42,79,170m3/h 增大时,升流区水平方向流速略有增加,沿水深方向流速增幅较大;直段流速随气量的增加变化不大;进气量大于79m3/h 后直段流速几乎没有变化,底部平均流速约为0.25m/s.通过测试不同进气量下的污泥浓度确定了保证流动的最小流速.进气量为20m3/h 时,沟内最大流速仅有0.07m/s,此时仍未出现污泥沉降.结合后续的污水处理效果研究,实际工程中可将沟底流速大于0.15m/s 作为防止污泥沉降的流速要求. 相似文献
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采用连续流动分析仪,用连续流动分光光度法,对水体中的氨氮进行实验研究。优化了试验方法,使氨氮的标准曲线线性相关性高,操作简便,大大提高了检测的效率,缩短了样品测量时间。样品中的测量值均在国家标准之内,测量的精度高。 相似文献
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在没有密度分层的容泄水体条件下,对某污水排海工程多孔喷头的射流特性进行了实验研究。文中介绍了不同排污流量和环境流速条件下,多孔喷头附近的流速场和污水场特性;并对出流平均稀释度作了分析。最后,还对该喷头周围的冲淤形态进行了探讨.文中所得的结果对实际排污系统的设计和进一步研究有一定的参考价值。 相似文献
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目的通过在开式空腔前缘增加矩形口射流、九孔射流和九斜孔射流,探究三种射流方式对空腔自激振荡噪声的抑制效果。方法通过风洞试验对亚、跨声速(Ma=0.3、0.45、0.6)下基于前缘射流的空腔噪声抑制方法开展研究,在空腔指定位置安装传声器,获取不同工况下空腔内的噪声信息,综合对比三种射流方式下空腔峰值频率、空腔底部及后壁声压级分布、总声压级分布及不同测点处的频率曲线特征,评估三种前缘射流方式对空腔噪声的控制效果。结果在来流速度Ma=0.3时,三种射流方式对空腔峰值频率处的声压级均有一定抑制效果,但由于前缘射流的引入导致空腔前端底部噪声总声压级提高;在来流速度Ma=0.45时,三种射流方式对空腔峰值频率处的声压级及宽频噪声均有显著抑制效果;在来流速度Ma=0.6时,除矩形口射流对空腔噪声有明显的抑制作用,其他两种射流方式使得空腔内噪声水平增强。结论在空腔前缘引入射流在一定来流速度下能够实现空腔峰值频率处噪声及宽频噪声的有效降低,前缘射流对空腔噪声的抑制效果随射流方式的不同而存在较大差异。 相似文献
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液幕湿法脱硫就是利用竖直向上喷射的石灰石浆液冲洗烟气,吸收效果好坏主要取决于喷嘴的竖直射流情况,试验研究了7种用于该塔中的喷嘴竖直射流特性。发现各喷嘴竖直射流都存在临界雾化速度。整理出无量纲平均半径与射流速度之间的关系,分析发现喷口直径和喷嘴高度对回落液体覆盖面积影响不大。试验结果表明所有喷嘴的回落液幕分布均匀性相同。导出了射流高度与喷射压力关系式,发现试验范围内喷嘴阻力损失情况相当。 相似文献
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目的 将空气幕自噪声问题简化为低亚声速大宽高比矩形射流噪声问题,并研究其特性。方法 设计低亚声速大宽高比矩形射流试验台,并系统地研究主要噪声来源以及射流速度、方位角、宽高比等参数对远场噪声的影响规律。结果 低亚声速大宽高比矩形射流远场噪声主要集中在低频部分(500 Hz以内),除宽高比为14的矩形射流噪声因声共振现象导致某些频率附近存在模态噪声峰值,从而不符合噪声频谱归一化规律外,其他低亚声速大宽高比矩形射流远场噪声频谱都符合如下规律,即射流噪声总声压级大致与射流速度的7.4次方成正比,与矩形喷管宽度的1.6次方成正比。结论 低亚声速大宽高比矩形射流远场噪声归一化规律可为深入了解空气幕自噪声特性提供理论指导。 相似文献
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采用声学多普勒测速仪(ADV)对水下推动器运行时氧化沟流场进行分析,结果表明:水下推动器单独运行时氧化沟直道流速分布规律与曝气转盘单独运行时不同,靠近叶轮处流速分布沿水深与沟宽都不同,可看作是一个点射流与典型明渠流动混合的流动,具有明显的三维性。通过一段距离的流速掺混,沟内液流可达到一个准二维流动。水下推动器安装在断面中部时的断面平均流速比安装在底部时大18%左右,动力利用率高,较有效地起到推流作用;安装在断面中部时紊动强度分布稳定时的断面离叶轮迎水面的相对距离比安装在断面底部短。 相似文献
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目的 研究药型罩结构参数对所形成的聚能射流在水中运动的影响,改进水中聚能射流的运动特性。方法 采用多物质单元ALE法就锥形罩射流对水介质的侵彻进行数值模拟,分析锥形装药结构中药型罩锥角和厚度对所形成的聚能射流侵彻水时运动参数的影响。结果 锥形罩锥角大小及药型罩厚度对聚能射流在水中的形状、射流速度、加速度等有着明显的影响。侵彻体进入水中10 cm后,药型罩的锥角从30°增加到150°的过程中,剩余速度先增大、后减小,在90°时达到最高。药型罩厚度为1.5~4mm时,剩余速度变化起伏小;厚度为4~6 mm时,剩余速度开始大幅下降。结论 当锥角为90°时,罩厚为4 mm的药型罩所形成的射流在水中表现最好,形成的射流侵彻深度最长,侵彻水介质10 cm后的剩余速度最大,存速能力最强。 相似文献
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Minimum quantity lubrication (MQL) is a cost-effective and environmentally friendly alternative to flood cooling. MQL spray jet has been shown to have potential to be applied successfully in different machining processes. Since the amount of lubricating liquid employed in MQL jet is very low, it is necessary to generate and apply the MQL spray efficiently. However, efficient application of MQL is not only related to spray atomization characteristics and delivery parameters but is also affected by machining conditions. The present paper demonstrates a theoretical and experimental investigation on the spray atomization and delivery parameters in the grinding process of Al2O3 engineering ceramics. The spray atomization characteristics studied are carrier gas velocity, liquid droplet size and liquid droplet velocity. Experiments were performed to verify the delivery parameters of MQL spray including nozzle angle, nozzle distance, lubricant flow rate and gas flow rate in the case of Al2O3 ceramics grinding. The experimental results confirm the theoretical outcomes and indicate that by applying optimal spray delivery parameters efficient lubrication takes place. Moreover, efficient lubrication of Al2O3 ceramics grinding can decrease the challenges existing in ceramics grinding processes by reducing grinding forces and surface roughness. 相似文献
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《Atmospheric Environment. Part A. General Topics》1991,25(7):1347-1375
Wind tunnel experiments and a theoretical model concerning the flow structure and pollutant diffusion over two-dimensional valleys of varying aspect ratio are described and compared. Three model valleys were used, having small, medium, and steep slopes. Measurements of mean and turbulent velocity fields were made upstream, within and downwind of each of these valleys. Concentration distributions were measured downwind of tracer sources placed at an array of locations within each of the valleys. The data are displayed as maps of terrain amplification factors, defined as the ratios of maximum ground-level concentrations in the presence of the valleys to the maxima observed from sources of the same height located in flat terrain. Maps are also provided showing the distance to locations of the maximum ground-level concentrations. The concentration patterns are interpreted in terms of the detailed flow structure measured in the valleys. These data were also compared with results of a mathematical model for treating flow and dispersion over two-dimensional complex terrain. This model used the wind tunnel measurements to generate mean flow fields and eddy diffusivities, and these were applied in the numerical solution of the diffusion equation. Measured concentration fields were predicted reasonably well by this model for the valley of small slope and somewhat less well for the valley of medium slope. Because flow separation was observed within the steepest valley, the model was not applied in this case. 相似文献