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1.
多排纵向涡发生器强化竖直平板自然对流换热的实验研究   总被引:1,自引:0,他引:1  
对多排纵向涡发生器对竖直平板自然对流的强化效果进行了研究。结果表明,在一定Rayleigh数范围内,直角三角翼纵向涡发生器的翼高、翼宽以及多排布置的阵列方式是影响强化换热的主要因素。在高宽比一定的情况下,存在最佳翼高。发现多排布置时LVG阵列方式的不同会影响换热效果;且要使得整个板的强化换热效果达到最佳,应选择沿竖直发热板长度方向间隔的布置多排LVG,并适当拉大间隔距离。  相似文献   

2.
将纵向涡强化换热技术应用于矩形管槽,研究以水为换热介质在过渡流状态下的换热效果。实验结果表明有纵向涡发生器的换热效果明显优于无纵向涡发生器的情况。利用PHEON ICS计算软件对实验进行数值模拟,模拟值与实验值符合较好。在此基础上,改变纵向涡的翼高和形状来模拟,发现两者均为换热影响的因素,相比之下,高宽比为0.4纵向涡发生器的换热效果比高宽比为0.5和0.6的要好。而采用相同高宽的矩形翼时,N u高于三角翼,但其换热性能指标却低于直角三角翼。  相似文献   

3.
新型矩形翼纵向涡发生器流动与换热实验研究   总被引:2,自引:0,他引:2       下载免费PDF全文
在矩形翼的侧面粘贴一个小矩形辅翼,构成一种新型矩形翼纵向涡发生器,称为组合翼。在压力损失相等的条件下,通过实验比较了矩形通道内组合翼与原始矩形翼纵向涡发生器的流动与换热特性。结果表明:对于原始矩形翼,其最佳攻角为45°;与矩形翼相比,组合翼的换热明显增强,且阻力系数减小,尤其当辅翼布置在矩形翼的上游时换热增强与阻力系数减小效果更加明显;研究范围内,辅翼攻角为30°时的流动与传热综合效果最佳。  相似文献   

4.
提出一种强化太阳能热风干燥器和集热器气侧换热的新型涡流发生器—斜截半椭圆柱体,并对其进行了实验研究及机理分析。在雷诺数为4000~38000的紊流范围内对矩形风道内分别布置单排一对直角三角翼、矩形翼、梯形翼、斜截半圆柱体、斜截半椭圆柱体等涡流发生器的强化传热效果和压降特性进行了对比实验。实验在稳态的气水逆流换热方式下进行,并固定各涡流发生器的高宽比为1/2,该迎流攻角为60°。结果表明,斜截半椭圆柱体是具有优越的强化气侧换热效果和低压降特性的新型涡流发生器。该对这种新型涡流发生器强化换热的机理作了初步分析。  相似文献   

5.
在矩形翼的基础上,提出一种新型的八边形翼纵向涡发生器.在矩形通道内,通过试验比较了矩形翼和八边形翼纵向涡发生器的流动与传热特性.分别在Re相同和阻力损失相同的条件下,分析了不同纵向涡发生器的强化传热效果.结果表明:与矩形翼相比,八边形翼纵向涡发生器的强化传热效果更好,而阻力系数没有明显增加;在阻力损失相同的条件下,矩形翼和八边形翼纵向涡发生器的传热增强率小于在Re相同时的传热增强率.  相似文献   

6.
纵向涡强化换热的优化设计及机理分析   总被引:1,自引:0,他引:1  
对带纵向涡发生器的椭圆管翅片换热器空气侧表面的换热和流动特性进行了三维数值模拟.深入分析了纵向涡对流场和温度场的影响,并通过场协同原理揭示了纵向涡强化换热的根本机理,即减小了速度和温度梯度之间的夹角,改善了速度场和温度场的协同性.在此基础上,对纵向涡发生器的布置位置(上游布置和下游布置)和纵向涡发生器的攻角α(15°,30°,45°,60°)进行了优化设计.结果表明:当纵向涡发生器布置于换热管下游时,具有更好的强化换热能力;在纵向涡发生器采用下游布置的前提下,当纵向涡发生器的攻角α=30°时,具有最佳的强化换热能力.  相似文献   

7.
采用三维数值模拟的方法研究了在片式散热器一组通道内设矩形涡流发生器(rectangualr vortex generator,RVGs)时对油侧的传热性能影响。研究了相同入口条件(层流)和考虑重力作用的条件下,纵向涡发生器的宽度、高度、攻角和纵向间距等几何因素对竖直通道传热和压降的影响。结果表明:纵向涡发生器产生的涡旋导致边界层分离,传热效果得到强化;改变涡发生器的宽度和高度对传热的影响趋势相似;当几何条件相同下攻角为30°时整体强化传热效果最佳;随着纵向间距的增加,传热的强化效果先降低再提高,最后又降低;最佳纵向间距为160 mm。  相似文献   

8.
利用三维数值模拟的方法对带有3种异形纵向涡发生器的H型翅片椭圆管换热器的空气侧流动传热特性进行研究。基于H型翅片椭圆管束,讨论了在不同雷诺数下,纵向涡发生器的摆放位置、摆放攻角和形状对空气侧流动传热的影响。研究表明:纵向涡发生器能够将高能量的流体引向流速较低的壁面区域,使冷热流体之间的混合加剧,增强流体的湍流动能,进而达到强化传热的效果;与无纵向涡发生器的管束相比,带纵向涡发生器管束的传热效果有明显的提高;当纵向涡发生器后置时,换热器的传热效果最优;在雷诺数相同,攻角为30°时,流体的传热性能和阻力特性均达到最优;相同攻角摆放时,椭圆角矩形发生器的传热性能和阻力因子均优于其他两种形式的发生器。研究结果为烟气余热回收系统换热器传热性能强化提供理论依据。  相似文献   

9.
为进一步提高管壳式换热器壳程换热效率,设计了一种布置于壳程肋片上的仿生鸟喙式涡流发生器。采用ANSYS FLUENT软件结合田口正交试验模拟了矩形通道中鸟喙式涡流发生器的传热特性,分析了纵向高度、斜截角度、迎流攻角、入口距离、流向间距5种结构参数对强化传热和综合热性能的贡献率及最佳结构组合。流动通道为长方体,其长、宽、高分别为1 600,240和40 mm,温度为286.86 K的空气流体从入口以1.491~3.195 m/s的速度流入,通道底部为337.048 K的恒温换热面。结果表明:纵向高度对于强化换热特性的贡献率最高,达到4744%,最强换热效果组合的换热因子较空矩形通道提高了185.71%;迎流攻角对于综合热性能的贡献率最高,达到了总占比的31.35%,利用正交试验分析得到的最强组合较空通道的综合热性能提高了47.82%  相似文献   

10.
外加电场强化苯自然对流和沸腾换热的试验研究   总被引:1,自引:0,他引:1  
对沉浸在非极性有机液体工质苯中的平板表面自然对流和沸腾换热的外加电场强化进行了试验,得出了自然对流和沸腾换热的换热系数、强化效果与电场电压、热流密度的关系。试验数据表明外加电场对平板表面苯的自然对流换热和沸腾换热都有一定的强化效果,但外加电场对平板表面苯自然对流换热的强化效果明显好于对沸腾换热的强化效果;且平板表面苯的自然对流换热的强化效果与试验所给定的热流密度无关,而外加电场对平板表面苯的沸腾换热的强化效果随热流密度的增大而减弱。  相似文献   

11.
This paper focuses on the study of heat transfer enhancement in natural vertical convection by using delta‐winglet longitudinal vortex generators. In the experimental range of Rayleigh numbers, the effect of attack angle, height, and width of the winglet of longitudinal vortex generator (LVG) on heat transfer performance was experimentally investigated. The results showed that there was an optimal attack angle and that the height and width can affect the heat transfer. In terms of array performance, it was shown that initial arrays could enhance the performance of later arrays. Moreover, the effects of LVG and low rectangular fins were compared. The results showed that the effect of LVGs was greater than that of low rectangular fins. © 2006 Wiley Periodicals, Inc. Heat Trans Asian Res, 35(6): 402–409, 2006; Published online in Wiley InterScience ( www.interscience.wiley.com ). DOI 10.1002/htj.20126  相似文献   

12.
3-D numerical simulations were presented for laminar flow and heat transfer characteristics in a rectangular channel with vortex generators. The effects of Reynolds number (from 800 to 3 000), the attack angle of vortex generator (from 15° to 90°) and the shape of vortex generator were examined. The numerical results were analyzed based on the field synergy principle. It is found that the inherent mechanism of the heat transfer enhancement by longitudinal vortex can be explained by the field synergy principle, that is, the second flow generated by vortex generators results in the reduction of the intersection angle between the velocity and fluid temperature gradient. The longitudinal vortex improves the field synergy of the large downstream region of longitudinal vortex generator (LVG) and the region near (LVG); however, transverse vortex only improves the synergy of the region near vortex generator. Thus, longitudinal vortex can enhance the integral heat transfer of the flow field, while transverse vortex can only enhance the local heat transfer. The synergy angle decreases with the increase of Reynolds number for the channel with LVG to differ from the result obtained from the plain channel, and the triangle winglet performs better than the rectanglar one under the same surface area condition.  相似文献   

13.
This paper presents the influences of main parameters of longitudinal vortex generator (LVG) on the heat transfer enhancement and flow resistance in a rectangular channel. The parameters include the location of LVG in the channel, geometric sizes and shape of LVG. Numerical results show that the overall Nusselt number of channel will decrease with the LVGs’ location away from the inlet of the channel, and decrease too with the space between the LVG pair decreased. The location of LVG has no significant influence on the total pressure drop of channel. With the area of LVG increased, the average Nusselt number and the flow loss penalty of channel, especially when β = 45° will increase. With the area of LVG fixed, increasing the length of rectangular winglet pair vortex generator will bring about more heat transfer enhancement and less flow loss increase than that increasing the height of rectangular winglet pair vortex generator. With the same area of LVG, delta winglet pair is more effective than rectangular winglet pair on heat transfer enhancement of channel, and delta winglet pair-b is more effective than delta winglet pair-a. Delta winglet pair-a results in a higher pressure drop, the next is rectangular winglet pair and the last is delta winglet-b. The increase of heat transfer enhancement is always accompanied with the decrease of field synergy angle between the velocity and temperature gradient when the parameters of LVG are changed. This confirms again that the field synergy is the fundamental mechanism of heat transfer by longitudinal vortex. The laminar heat transfer of the channel with punched delta winglet pair is experimentally and numerically studied in the present paper. The numerical result for the average heat transfer coefficient of the channel agrees well with the experimental result, indicating the reliability of the present numerical predictions.  相似文献   

14.
The heat transfer enhancement of the longitudinal vortex (LV) is a kind of technology with high efficiency and low thermal resistance. An LV is produced by longitudinal vortex generators (LVGs). Due to their relative long influence distance and simple structure, the LVGs may be used in narrow channels with a flat surface. In this paper, the dimension of a narrow rectangular channel is 600 mm (length) × 40 mm (width) × 3 mm (height), and one LVG is 14 mm (length) ×2.2 mm (width) × 1.8 mm (height). The rectangular blocked LVGs are periodically laid out in the heated plate, and the attack angle of LVGs is 44°, the longitudinal pitch between LVGs is 100 mm, and the transverse pitch between LVGs is 4 mm. The test section is visual with three surfaces and heated with one surface by direct current. The working fluid is water. The experimental results show that the boiling heat transfer coefficient on the heated surface is increased by 25.8%, while the pressure drop along the test section is increased by 50.6%. At the same time, the visual experimental data shows that the bubbles’ behavior has been intensively affected by LVs, the growth and gathering of bubbles have been depressed, and the thermal boundary layer in the test section has been greatly damaged and reduced; as results, the momentum and energy exchange in the test section have been strengthened. Thus, the heat transfer is obviously enhanced by LVs.  相似文献   

15.
This study presents numerical computation results on laminar convection heat transfer in a rectangular channel with a pair of rectangular winglets longitudinal vortex generator punched out from the lower wall of the channel. The effect of the punched holes and the thickness of the rectangular winglet pair to the fluid flow and heat transfer are numerically studied. It is found that the case with punched holes has more heat transfer enhancement in the region near to the vortex generator and lower average flow frictional coefficient compared with the case without punched holes. The thickness of rectangular winglet can cause less heat transfer enhancement in the region near to the vortex generator and almost has no significant effect on the total pressure drop of the channel. The effects of Reynolds number (from 800 to 3000), the attack angle of vortex generator (15°, 30°, 45°, 60° and 90°) were examined. The numerical results were analyzed from the viewpoint of field synergy principle. It was found that the essence of heat transfer enhancement by longitudinal vortex can be explained very well by the field synergy principle, i.e., when the second flow generated by vortex generators results in the reduction of the intersection angle between the velocity and fluid temperature gradient, the heat transfer in the present channels will be enhanced. Longitudinal vortices (LVs) improve the synergy between velocity and temperature field not only in the region near LVG but also in the large downstream region of longitudinal vortex generator. So LVs enable to enhance the global heat transfer of channel. Transverse vortices (TVs) only improve the synergy in the region near VG. So TVs can only enhance the local heat transfer of channel.  相似文献   

16.
Longitudinal vortices are capable of producing beneficial effects in heat transfer enhancement. Experiments in natural convection heat transfer enhancement were done on a vertical flat heating plate using delta‐winglet longitudinal vortex generators (LVGs) arranged in rows. In an experimental range of Rayleigh number, the height and width of the winglet of the longitudinal vortex generator (LVG), the array form of the longitudinal vortex generators on the heat transfer performance were experimentally investigated, and the best height of the winglet of the longitudinal vortex generator was obtained. The results showed the change of the array form of the longitudinal vortex generators could affect the heat transfer effect. Finally by arranging some longitudinal vortex generator arrays with the appropriate interval, the whole heat transfer effect of the interval could reach a prime value. © 2006 Wiley Periodicals, Inc. Heat Trans Asian Res, 35(5): 351–358, 2006; Published online in Wiley InterScience ( www.interscience.wiley.com ). DOI 10.1002/htj.20119  相似文献   

17.
3-D numerical simulations were presented for laminar flow and heat transfer characteristics in a rectangular channel with vortex generators. The effects of Reynolds number (from 800 to 3 000), the attack angle of vortex generator (from 15° to 90°) and the shape of vortex generator were examined. The numerical results were analyzed based on the field synergy principle. It is found that the inherent mechanism of the heat transfer enhancement by longitudinal vortex can be explained by the field synergy principle, that is, the second flow generated by vortex generators results in the reduction of the intersection angle between the velocity and fluid temperature gradient. The longitudinal vortex improves the field synergy of the large downstream region of longitudinal vortex generator (LVG) and the region near (LVG); however, transverse vortex only improves the synergy of the region near vortex generator. Thus, longitudinal vortex can enhance the integral heat transfer of the flow field, while transverse vortex can only enhance the local heat transfer. The synergy angle decreases with the increase of Reynolds number for the channel with LVG to differ from the result obtained from the plain channel, and the triangle winglet performs better than the rectanglar one under the same surface area condition. __________ Translated from Journal of Xi’an Jiaotong University, 2006, 40(9): 996–1000 [译自: 西安交通大学学报]  相似文献   

18.
This study presents numerical computation results on laminar convection heat transfer in a plate‐fin heat exchanger, with triangular fins between the plates of a plate‐fin heat exchanger. The rectangular winglet type vortex generator is mounted on these triangular fins. The performance of the vortex generator is evaluated for varying angles of attack of the winglet i.e., 20, 26, and 37° and Reynolds number 100, 150, and 200. The computations are also performed by varying the geometrical size and location of the winglet. The complete Navier–Stokes equation and the energy equation are solved by the (Marker and Cell) MAC algorithm using the staggered grid arrangement. The constant wall temperature thermal boundary conditions are considered. Air is taken as the working fluid. The heat transfer enhancement is seen by introducing the vortex generator. Numerical results show that the average Nusselt number increases with an increase in the angle of attack and Reynolds number. For the same area of the LVG, the increase in length of the LVG brings more heat transfer enhancement than increasing the height. The increase in heat transfer comes with a moderate pressure drop penalty. © 2010 Wiley Periodicals, Inc. Heat Trans Asian Res; Published online in Wiley Online Library ( wileyonlinelibrary.com ). DOI 10.1002/htj.20318  相似文献   

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