共查询到17条相似文献，搜索用时 140 毫秒
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考虑环境湍流作用的烟气上升路径方程 总被引：1，自引：3，他引：1
本文利用我国的观测资料对中性层结时的烟气拾升路径作了细致的分析。发现抬升高度与距离之间符合幂次关系,但与不考虑环境湍流作用的2/3次律有系统偏离;这一偏离与烟流半径和高度的非线性关系相一致。上述事实与国外的一些观测结果均表明,环境湍流对烟气抬升的累积作用不容忽视。为此,提出了环境湍流与自生湍流的联合作用模式,由此导得的抬升路径方程可以满意地解释上述观测事实。模式还显示,卷挟速度除取决于切变速度及湍流强度以外,还是烟流半径的函数,因而在物理上更加合理。由联合作用模式导出的终极抬升公式比不考虑环境湍流累积作用的公式更符合观测结果。 相似文献
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对强浮升烟流,采用通常意义上确定的抬升高度计算污染物浓度分布尤其是地面最大浓度会造成较大的误差。我们认为此时应取地面浓度达最大值处为烟流抬升的截止点。在这一假设条件下,本文得出了强浮升烟流的终极抬升高度计算公式和地面最大浓度距离计算公式。美国PPSP试验资料验证了我们的主要结论。 相似文献
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本文通过Boussinesq近似的非线性动力方程组,得到了烟流抬升高度的解析表达式,讨论了地形、大气稳定度等物理因子对烟流抬升高度的影响。结果表明:地形的分布对烟流抬升高度的确定有一定影响,大气稳定度对高度的影响尤为明显。本文还讨论了理论公式的实用条件。 相似文献
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考虑环境湍流对烟气抬升具有增强烟气夹卷和促进烟气与环境空气间动、热量交换的双重作用，导出了中性层结条件下热烟气浮升的轨迹方程，并且无需对抬升的截止作任何假设，导得了理论的终极抬升公式。经与国内外烟气抬升实测资料对比，发现这些结果与实况基本一致。 相似文献
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本文叙述了1987年5月8日大兴安岭森林火灾烟羽形成的气象背景,由卫星烟羽照片计算了行走时间在6×10~4s以内的瞬时烟羽扩散参数。计算结果表明长度为100km的烟流瞬时扩散较接近线性律,更长的烟流则对3/2律符合得更好些,此外还用烟团抬升公式估计了5月7至8日大火的热释放量,计算值能与现场调查值在量级上相一致。 相似文献
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本文用积云一维定常模式摸拟烟囱烟流抬升状况,用数值实验的方式摸拟和计算烟气在静稳条件下的抬升高度,从另一个角度给出了烟气抬升研究的方法。 相似文献
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对几种烟云抬升模式进行了比较,分析了中性层结下环境湍流的对烟云抬升的作用,认为环境流连续作用于烟云抬升的各个阶段,且随烟云抬升而变化。抬升高度与环境湍流有关,湍流强度越大,抬升越低。 相似文献
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利用2018年6月2日至2019年11月14日,安庆、长沙、赣州、南昌、宜昌、武汉6个站点的往返式探空试验数据,使用Thorpe分析方法计算了湍流层厚度、对数湍流耗散率、Thorpe尺度、浮力频率并进行概率、水平、垂直等分布特征的分析。这些探空数据观测精度较高,且垂直分辨率约为6～10 m,延伸至大约30 km的高度,可以在整个对流层和平流层下部估计湍流。本研究基于湍流特征分析,比较了各个站点之间以及上升段与下降段之间的差异。对数湍流耗散率log10ε(代表ε的量级)分布具有两个模态,分别以-35 m2 s-3和-5 m2 s-3附近为峰值中心并向两侧递减。对流层的分布相对于平流层更加集中,且对流层的峰值中心的数值略大于平流层中心,这说明平流层的湍流强度稍弱于对流层。从对数湍流耗散率log10ε、Thorpe尺度(LT)、浮力频率(N2)三个参数的水平和垂直分布可以看出,湍流强度受LT与N<... 相似文献
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Considering the effects of both entrainment and intensification of the exchanges of momentum and heat between plume and ambient air,we have derived the trajectory equation of buoyant plume under neutral conditions,and the final rise prediction formula theoretically without any hypotheses on the rise termination.Compared with the field experiments,the final rise formula simulates the observed final rise heights well. 相似文献
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This paper has investigated the rise of bent-over buoyant plume in neutral condition.By means of the combined-effect model proposed at earlier time,authors have deduced a formula of final rise limited by mechanical turbulence and therefore have concluded that the corresponding formula neglecting the accumulated effect of ambient turbulence is only its particular case.By analyzing the function relation of the various affecting factors with the plume rise in the existing equations,it is proved that the formula derived from the combined-effect model is the most reasonable and shows more conformity to the observations. 相似文献
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Experimental data for buoyant plumes released from high sources into layers having little ambient turbulence show that plume dispersion parameters vary in a manner similar to that during initial plume rise. This is consistent with general plume rise theory. Dispersion of plumes from tall stacks in a shoreline environment where a thermal internal boundary layer is formed often demonstrates this behaviour. 相似文献
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环境湍流对烟云抬升的作用 总被引：2，自引：1，他引：2
本文研究了中性层结环境中湍流对烟云抬升的连续作用。取外部湍流卷挟率正比于湍流特征速度并叠加于自身卷挟率,分析表明,即使在抬升的早期,环境湍流对弯曲烟云的路径有不可忽视的影响,并使烟云路径加速变平。电厂烟云的实测资料表明,平均抬升路径实际上不完全符合无湍流环境的三分之二规律,而与本文理论结果更为接近。 本研究也发现,最大抬升高度及其出现的下风距离都是大气湍流度的灵敏函数。据此,我们分析了几个常用抬升公式的局限性,并推荐了一种反映大气湍流度的改型公式。 相似文献
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Field and laboratory studies have been conducted to investigate the effect of surrounding buildings on the plume rise from low-level buoyant sources, such as distributed power generators. The field experiments were conducted in Palm Springs, California, USA in November 2010 and plume rise from a 9.3 m stack was measured. In addition to the field study, a laboratory study was conducted in a water channel to investigate the effects of surrounding buildings on plume rise under relatively high wind-speed conditions. Different building geometries and source conditions were tested. The experiments revealed that plume rise from low-level buoyant sources is highly affected by the complex flows induced by buildings stationed upstream and downstream of the source. The laboratory results were compared with predictions from a newly developed numerical plume-rise model. Using the flow measurements associated with each building configuration, the numerical model accurately predicted plume rise from low-level buoyant sources that are influenced by buildings. This numerical plume rise model can be used as a part of a computational fluid dynamics model. 相似文献
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Han Van Dop 《Boundary-Layer Meteorology》1993,62(1-4):97-105
For the dispersion of buoyant material, the interaction with the environment by entrainment forms a serious obstacle for a formulation in a Lagrangian framework. Nevertheless an outline is given here on how buoyant plume rise in a Lagrangian sense could be described. Though the method contains a number of heuristic elements, it has all the advantages of a Lagrangian formulation. It is shown that it is possible to formulate a Lagrangian model which both is able to recover the classical formulations for plume rise in a calm environment and to accomodate more recent Eulerian formulations in a turbulent environment. Moreover, the method offers excellent possibilities to include the turbulent characteristics of the plume's environment and arbitrary stratifications of the boundary layer. These facts make it attractive for various practical applications. Some examples are given which illustrate this. 相似文献
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Mesoscale measurements of the vertical dispersion coefficient 2 by using a composite turbulence water tank were validated through a comparison with CONDORS (Convective Diffusion Observed with Remote Sensors) field data, and were analysed with respect to the intensity of the thermal flux, mechanical turbulence, and plume release height.It seems possible to correct the plume z values for different release heights below 0.5zi (zi is the mixing height) by applying an equation expressing the height dependency of turbulence intensity. The downwind distance where the plume's mass centre height approaches its final level was also analysed with respect to the above three parameters, and an empirical equation to estimate the downwinddistance derived. 相似文献