共查询到19条相似文献,搜索用时 171 毫秒
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针对我国北方冬季湿式冷却塔运行时填料下表面、进风口以及基环面等处容易结冰的问题,在冷却塔的进风口处加装挡风板,建立了冷却塔内的传热传质模型,并采用CFD软件模拟和分析了在不同横向风速和不同环境温度下加装不同层数的挡风板时冷却塔的热力特性.结果表明:在风速小于4m/s时,塔内的迎风面空气温度较低,极易结冰;随着风速的增大,低温区逐渐向背风侧转移;当风速为8m/s,环境温度分别为-10℃、-17℃、-23℃时,分别在冷却塔内加装1层、3层和5层挡风板,能大大改善塔内温度场,有效防止塔内结冰. 相似文献
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由于我国北方地区冬季气温较低,冷却塔普遍存在结冰问题,必须采取一定的防冻措施。通过FLUENT软件模拟分析得出进塔水温对塔内不同特征面水温的影响规律,并进一步模拟加装不同层数挡风板后冷却塔内流场的变化。计算结果表明:①当运行工况其它条件不变时,随着进塔水温的升高,塔内不同特征面最低水温升高;②加装一定层数挡风板能使填料下面空气温度场和进风口上沿面空气速度场分布逐渐趋于均匀,有利于防止塔内结冰;③选取进塔水温分别为17.80℃、21.95℃、26.77℃、30.04℃时,分别加装4、3、2、1层挡风板可有效防止塔内结冰。 相似文献
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《汽轮机技术》2016,(5)
冷却塔作为火电厂冷端系统中重要的冷却设备之一,其冷却性能直接影响电厂运行的安全稳定性和经济性,而环境侧风在很大程度上影响冷却塔的冷却性能,可以采取在冷却塔进风口处安装导流板的措施予以改善。针对某600MW机组的自然通风湿式冷却塔,采用CFD软件Fluent,对进风口处安装导流板的冷却塔进行数值模拟。模拟结果表明:导叶板能够增加塔内中心区域的空气上升速度和扰动,加强传热,改善冷却塔冷却性能。导叶板相对最佳的安装角度为20°,导叶板安装数量为80块,出塔水温可以降低1.2K。根据模拟结果对某冷却塔进行改造,通过对比同一塔技改前后出塔水温,发现出塔水温可降低1.6K以上,验证了模拟计算的正确性和该项技术的实用性。 相似文献
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《汽轮机技术》2015,(1)
基于RNG k-ε湍流模型和多孔介质模型,对SCAL型自然通风冷却塔的内部流场进行了三维数值模拟,并分析了风速和温度对空冷塔通风量的影响规律。计算结果表明,风速和温度分别为6m/s和42℃时为最不利环境工况。针对不利工况提出了在空冷塔内加装喷嘴组和外接气源的优化措施,并进行了加装装置前后塔内流场特性的数值模拟。结果表明,加装喷气装置后塔内流场明显改善,且通风量增大;综合分析优化结果、运行成本以及可操作性,在进风口截面安装48个喷嘴且流量为0.005kg/s为最理想方案,塔内通风量增加8.259%。该方案对解决电厂间接空冷机组夏季出力不足等问题具有重要的理论意义和工程价值。 相似文献
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通过对某企业供排水车间冷却塔应用进风口填料斜角技术实际项目进行的监测、研究和效益分析,得出冷却塔应用进风口填料斜角技术可达到节能效果的结论。 相似文献
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对于基坑式环境,在环境风与冷却塔风机抽力的作用下,冷却塔出风口排出的热空气易被冷却塔进风口再次吸入塔内,形成热风回流,导致冷却塔实际冷效低于设计值。以某会议会展工程为例,通过CFD热流模拟,在基坑式环境下对冷却塔进行合理选型,根据气流组织模拟确定冷却塔的布置位置、方向以及基础高度,保证冷却塔使用能效优良。 相似文献
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《Applied Thermal Engineering》2007,27(5-6):910-917
Cooling towers are used to extract waste heat from water to atmospheric air. An energy analysis is usually used to investigate the performance characteristics of cooling tower. However, the energy concept alone is insufficient to describe some important viewpoints on energy utilization. In this study, an exergy analysis is used to indicate exergy and exergy destruction of water and air flowing through the cooling tower. Mathematical model based on heat and mass transfer principle is developed to find the properties of water and air, which will be further used in exergy analysis. The model is validated against experimental data. It is noted from the results that the amount of exergy supplied by water is larger than that absorbed by air, because the system produces entropy. To depict the utilizable exergy between water and air, exergy of each working fluid along the tower are presented. The results show that water exergy decreases continuously from top to bottom. On the other hand, air exergy is expressed in terms of convective and evaporative heat transfer. Exergy of air via convective heat transfer initially loses at inlet and slightly recovers along the flow before leaving the tower. However, exergy of air via evaporative heat transfer is generally high and able to consume exergy supplied by water. Exergy destruction is defined as the difference between water exergy change and air exergy change. It reveals that the cooling processes due to thermodynamics irreversibility perform poorly at bottom and gradually improve along the height of the tower. The results show that the lowest exergy destruction is located at the top of the tower. 相似文献
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《International Communications in Heat and Mass Transfer》2005,32(8):1066-1074
In the present study, both experimental and theoretical results of the heat transfer characteristics of the cooling tower are investigated. A column packing unit is fabricated from the laminated plastic plates consists of eight layers. Air and water are used as working fluids and the test runs are done at the air and water mass flow rates ranging between 0.01 and 0.07 kg/s, and between 0.04 and 0.08 kg/s, respectively. The inlet air and inlet water temperatures are 23 °C, and between 30 and 40 °C, respectively. A mathematical model based on the conservation equations of mass and energy is developed and solved by an iterative method to determine the heat transfer characteristics of the cooling tower. There is reasonable agreement from the comparison between the measured data and predicted results. 相似文献
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The Hybrid Ground Source Heat Pump (GSHP) systems combine the renewable geothermal energy and cooling tower for rejecting the cooling load, which is often adopted for high cooling demand. Model based control can be limited due to variations in ambient conditions, ground-loop heat exchanger (GHE) and equipment characteristics, cost and reliability of sensors. A self-optimizing control scheme is proposed for efficient operation of the hybrid GSHP based on Extremum Seeking Control (ESC), with feedback of the total power consumption and the control inputs of the relative flow rate of cooling tower and the water pump speed. The cooling capacity of the heat pump regulates the evaporator leaving water at 7 °C. A Modelica based dynamic simulation model is developed for a Hybrid GSHP system, with the vertical GHE model adopted from Modelica Buildings Library. The transient heat transfer is implemented with a finite volume method inside and outside the borehole. The proposed ESC scheme is evaluated under the scenarios of fixed cooling load, ramp change in the evaporator inlet water temperature, diurnal sinusoidal cycle of air wet-bulb temperature, and realistic ambient and cooling load condition. Simulation results show the proposed ESC strategy effectively achieves nearly optimal efficiency without the need for plant model. 相似文献
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为了分析不同风量和喷淋水量对填料逆流闭式冷却塔热力性能的影响,建立和验证了带填料逆流闭式冷却塔热质交换的数学模型,基于焓差理论对模型计算的结果进行分析。结果表明:加入填料相当于对盘管区进口的喷淋水进行预冷,降低了喷淋水的平均温度,使带填料闭式冷却塔的冷却性能优于纯盘管闭式冷却塔;风量的增加可以提高带填料逆流闭式冷却塔和纯盘管逆流闭式冷却塔的热力性能,两种塔的冷却性能随风量增加的提升速率相同;喷淋水量的增加对纯盘管逆流闭式冷却塔的热力性能的影响较小,却可以较大幅度提高带填料逆流闭式冷却塔的热力性能。 相似文献
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《Applied Thermal Engineering》2001,21(9):899-915
In this paper, a mathematical model for a counterflow wet cooling tower is derived, which is based on one-dimensional heat and mass balance equations using the measured heat transfer coefficient. The balance equations are solved numerically to predict the temperature change of air and water, as well as the humidity as a function of the cooling tower high. Experimental measurements on two pilot-scale cooling towers were carried out in order to analyze the performance of different cooling tower filling materials. Also, the performance of other cooling tower elements, such as droplet separators and water spray nozzles, was investigated in the pilot experiments. The flow distribution, i.e. the velocity field, upstream to the filling material was predicted using the three-dimensional version of the computational fluid dynamics (CFD) code Fluent/uns, version 4.2. The calculated flow fields are presented for different distances between the inlet of the air and the filling material. In addition, the two-dimensional version of the CFD code Fluent/uns, version 4.2, was applied to predict the external airflow around the cooling tower and the backflow in different weather conditions in summer and winter. The research project was carried out in connection to an industrial cooling tower installation. 相似文献
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A method is proposed for predicting the variations of air and water temperatures and of air humidity in a packed bed counterflow type of cooling tower subjected to a thermal disturbance. Heat input-response measurements are carried out by imposing thermal disturbances on inlet water and inlet air. The air-film and water-film heat transfer coefficients are estimated by fitting in the time domain the measured output temperature/humidity variations to those predicted. 相似文献
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Transfer characteristic correlations given in the literature for wet-cooling tower fills are generally only a function of the air and water mass flow rates. This is a gross simplification of a very complex heat and mass transfer (evaporative cooling) process. In addition to the effects of the air and water mass flow rates, effects of the inlet water temperature, air drybulb temperature, wetbulb temperature, and fill height on the transfer characteristic, or Merkel number, are investigated in the present study. The accuracy of two different empirical equations is also evaluated. It is found that the transfer characteristic correlations for wet-cooling tower fills are functions of the inlet water temperature and fill height but not of the air drybulb and wetbulb temperatures. 相似文献