CN101644545B - Air-cooled condenser - Google Patents
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- 239000002826 coolant Substances 0.000 claims abstract description 4
- 239000000919 ceramic Substances 0.000 claims description 32
- 229910052451 lead zirconate titanate Inorganic materials 0.000 claims description 5
- 239000002184 metal Substances 0.000 claims description 4
- 229910052751 metal Inorganic materials 0.000 claims description 4
- 239000006104 solid solution Substances 0.000 claims description 3
- HWHWBMBTCNLBGY-UHFFFAOYSA-N [Pb].[Ni].[Nb] Chemical compound [Pb].[Ni].[Nb] HWHWBMBTCNLBGY-UHFFFAOYSA-N 0.000 claims description 2
- 238000001816 cooling Methods 0.000 abstract description 19
- 230000017525 heat dissipation Effects 0.000 abstract description 15
- 238000005516 engineering process Methods 0.000 abstract description 4
- 230000000694 effects Effects 0.000 description 19
- 238000006073 displacement reaction Methods 0.000 description 6
- 230000007423 decrease Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 239000000243 solution Substances 0.000 description 4
- 230000005684 electric field Effects 0.000 description 3
- 238000005265 energy consumption Methods 0.000 description 3
- 238000004088 simulation Methods 0.000 description 3
- 239000012530 fluid Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 230000003321 amplification Effects 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 229910010293 ceramic material Inorganic materials 0.000 description 1
- 239000003245 coal Substances 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000008602 contraction Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 230000005284 excitation Effects 0.000 description 1
- 238000012417 linear regression Methods 0.000 description 1
- 238000004377 microelectronic Methods 0.000 description 1
- FEBJSGQWYJIENF-UHFFFAOYSA-N nickel niobium Chemical compound [Ni].[Nb] FEBJSGQWYJIENF-UHFFFAOYSA-N 0.000 description 1
- 238000003199 nucleic acid amplification method Methods 0.000 description 1
- 230000010287 polarization Effects 0.000 description 1
- 238000005498 polishing Methods 0.000 description 1
- 230000005855 radiation Effects 0.000 description 1
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Abstract
本发明涉及空冷技术领域,一种空冷冷凝器,具有输送冷却介质的散热管,并沿散热管布置有压电式风扇。本发明与现有技术相比具有功耗低,噪音小,换热能力强等优点。
The invention relates to the field of air-cooling technology, and relates to an air-cooled condenser, which has a heat dissipation pipe for conveying a cooling medium, and a piezoelectric fan is arranged along the heat dissipation pipe. Compared with the prior art, the invention has the advantages of low power consumption, low noise, strong heat exchange capacity and the like.
Description
技术领域technical field
本发明涉及空冷技术领域,特别是一种使用压电式风扇的空冷冷凝器。The invention relates to the technical field of air cooling, in particular to an air cooling condenser using a piezoelectric fan.
背景技术Background technique
空冷技术作为一项经济而又相对环保的节水途径,成为解决在“富煤缺水”地区或干旱地区建设火力发电厂的一个重要选择。然而,迄今为止的直接空冷机组主要是依靠大型轴流风机产生受迫对流,其能耗大,噪音大,易受环境风的影响。As an economical and relatively environmentally friendly water-saving approach, air-cooling technology has become an important choice to solve the construction of thermal power plants in "coal-rich and water-shortage" areas or arid areas. However, the direct air-cooling units so far mainly rely on large axial flow fans to generate forced convection, which consumes a lot of energy, is noisy, and is easily affected by ambient wind.
压电效应是一个一百多年前就已经认识的物理现象,通过这一效应,某些特殊陶瓷材料可以在外加电场的激励下产生很大的机械应力。不过,压电效应所直接产生的形变或位移通常都很小,因而长期以来主要被用作压力传感器以及微纳米器件的执行器。利用压电效应产生明显的空气流动是应微电子设备冷却的需要而在近10年内发展起来的,用以解决智能手机,DVD播放机等声音敏感设备散热风扇的噪音问题。迄今为止,其并未能应用于空冷技术中。The piezoelectric effect is a physical phenomenon known more than one hundred years ago. Through this effect, certain special ceramic materials can generate large mechanical stress under the excitation of an external electric field. However, the deformation or displacement directly produced by the piezoelectric effect is usually very small, so it has been mainly used as a pressure sensor and an actuator for micro-nano devices for a long time. The use of the piezoelectric effect to generate significant air flow was developed in the past 10 years in response to the cooling needs of microelectronic devices to solve the noise problem of cooling fans for sound-sensitive devices such as smartphones and DVD players. So far, it has not been applied in air cooling technology.
发明内容Contents of the invention
本发明的目的是为了克服上述背景技术的不足之处,提供一种利用功能陶瓷的逆压电效应带动振动片取代空冷风机使空气振荡换热的冷凝器,其功耗低,噪音小,换热能力强。The purpose of the present invention is to overcome the shortcomings of the above-mentioned background technology, and provide a condenser that uses the inverse piezoelectric effect of functional ceramics to drive the vibrating plate to replace the air-cooling fan to make the air oscillate and exchange heat, which has low power consumption and low noise. Strong heat capacity.
本发明的目的是通过如下技术措施来实现的:一种空冷冷凝器,具有输送冷却介质的散热管,其沿散热管布置有压电式风扇。The object of the present invention is achieved through the following technical measures: an air-cooled condenser has a heat dissipation pipe for conveying a cooling medium, and a piezoelectric fan is arranged along the heat dissipation pipe.
在上述技术方案中,所述压电式风扇包括由金属薄片制成的叶片和固定在叶片边缘上的压电陶瓷片,压电陶瓷片的另一端固定在与散热管邻近的支撑架上,各压电陶瓷片与一交变电源相并联。In the above technical solution, the piezoelectric fan includes blades made of thin metal sheets and piezoelectric ceramic sheets fixed on the edges of the blades, and the other end of the piezoelectric ceramic sheets is fixed on a support frame adjacent to the heat dissipation pipe, Each piezoelectric ceramic sheet is connected in parallel with an alternating current power supply.
在上述技术方案中,所述压电式风扇上的压电陶瓷片为一个或为厚度相同叠合起来的多个。In the above technical solution, the piezoelectric ceramic sheet on the piezoelectric fan is one or a plurality of stacked ones with the same thickness.
在上述技术方案中,所述叶片与散热管的距离为0.05~0.15米,各压电陶瓷片之间的距离为0.1~0.3米,叶片自压电陶瓷片的延伸长度(即下文所述的叶片长度)为0.3~0.7米。In the above technical solution, the distance between the blade and the heat pipe is 0.05 to 0.15 meters, the distance between each piezoelectric ceramic sheet is 0.1 to 0.3 meters, and the extension length of the blade from the piezoelectric ceramic sheet (that is, the length described below) Leaf length) is 0.3 to 0.7 meters.
在上述技术方案中,所述压电陶瓷片是铌镍锆钛酸铅(PZT)为主要成分的固熔体。In the above technical solution, the piezoelectric ceramic sheet is a solid solution of lead niobium nickel zirconate titanate (PZT) as the main component.
本发明利用功能陶瓷的逆压电效应,把电能转换为机械能,同时通过压电陶瓷片与叶片的共振把压电效应产生的微尺度振动以非常低的耗能转变为宏观尺度的振动,以产生足够流量的空气流动达到空冷换热的目的,并且将共振的频率选择在听觉所能感觉的频率之外,几乎可以完全消除噪音的影响。与现有技术相比本发明的优点在于功耗低,噪音小,换热能力强。The invention uses the inverse piezoelectric effect of functional ceramics to convert electrical energy into mechanical energy, and at the same time converts the micro-scale vibration generated by the piezoelectric effect into macro-scale vibration with very low energy consumption through the resonance between the piezoelectric ceramic sheet and the blade. The air flow that generates enough flow can achieve the purpose of air cooling and heat exchange, and the frequency of resonance is selected outside the frequency that can be felt by hearing, which can almost completely eliminate the influence of noise. Compared with the prior art, the invention has the advantages of low power consumption, low noise and strong heat exchange capacity.
附图说明Description of drawings
图1为本发明实施例结构示意图。Fig. 1 is a schematic structural diagram of an embodiment of the present invention.
图2为实施例中压电式风扇结构示意图。Fig. 2 is a schematic structural diagram of the piezoelectric fan in the embodiment.
图3为应用本发明的压电空冷系统框图。Fig. 3 is a block diagram of a piezoelectric air cooling system applying the present invention.
图4为基于本发明的空冷冷凝器的布置结构图。Fig. 4 is an arrangement diagram of an air-cooled condenser based on the present invention.
图5为叶片到散热管距离与管壁表面传热系数的关系图。Fig. 5 is a graph showing the relationship between the distance from the blade to the heat pipe and the heat transfer coefficient of the pipe wall surface.
图6为叶片间距与管壁表面传热系数的关系图。Fig. 6 is a graph showing the relationship between the blade pitch and the heat transfer coefficient of the tube wall surface.
图7为叶片长度与管壁表面传热系数的关系图。Fig. 7 is a graph showing the relationship between the blade length and the heat transfer coefficient of the tube wall surface.
图8为叶片工作频率与管壁表面传热系数的关系图。Fig. 8 is a graph showing the relationship between the operating frequency of the blade and the heat transfer coefficient of the tube wall surface.
图9为叶片布置方式与管壁表面传热系数的关系图。Fig. 9 is a graph showing the relationship between the arrangement of blades and the heat transfer coefficient of the tube wall surface.
其中,1为散热管,2为压电陶瓷片,3为叶片,4为支撑架,5为锅炉,6为过热器,7为汽轮机,8为发电机,9为汽轮机排汽管道,10为散热管,11为冷却元件,12为小型电动机,13为凝结水箱,14为凝结水泵,15为凝结水精处理装置,16为凝结水泵,17为低压加热器,18为除氧器,19为给水泵,20为高压加热器。Among them, 1 is the cooling pipe, 2 is the piezoelectric ceramic sheet, 3 is the blade, 4 is the support frame, 5 is the boiler, 6 is the superheater, 7 is the steam turbine, 8 is the generator, 9 is the exhaust pipe of the steam turbine, 10 is Radiation pipe, 11 is cooling element, 12 is small motor, 13 is condensate tank, 14 is condensate pump, 15 is condensate polishing device, 16 is condensate pump, 17 is low pressure heater, 18 is deaerator, 19 is Feedwater pump, 20 is a high-pressure heater.
具体实施方式Detailed ways
下面结合说明书附图对本发明作进一步的描述。The present invention will be further described below in conjunction with the accompanying drawings.
如图1所示,本实施例中所述空冷冷凝器,具有输送冷却介质的散热管1,其沿散热管1布置有压电式风扇。As shown in FIG. 1 , the air-cooled condenser in this embodiment has a
如图2所示,所述压电式风扇包括由金属薄片制成的叶片3和固定在叶片3边缘上的压电陶瓷片2,压电陶瓷片2的另一端固定在与散热管1邻近的支撑架4上,各压电陶瓷片2与一交变电源相并联,其电源接线沿着金属支撑架4安装,由变压器和电阻R控制置于压电风扇两端的电压。As shown in Figure 2, the piezoelectric fan includes a
所述压电陶瓷片2是铌镍锆钛酸铅(PZT)为主要成分的固熔体。其两面形成电极,极化方向与电极垂直,如果在压电陶瓷片2的电极间加上电压,由于逆压电效应,则压电陶瓷片2的振子便会在长度方向产生位移。采用多层压电陶瓷片2结构,是把几层厚度相同的压电陶瓷片2,叠合成叠层体,并在电气上并联和机械上串联构成,加上电场时在长度方向伸长,它的总位移量为每层位移量的几倍。这种结构推力很大,且因有机械增益,它们的位移量都大于块体的涨缩位移,所以有较大的偏转位移。The piezoelectric
本专利就是利用压电陶瓷片2的逆压电效应,采取压电陶瓷片2与叶片3共振放大的方法,将压电陶瓷片2的微尺度振动放大2-3个数量级以产生大规模的空气流动,从而代替传统直接空冷机组中的驱动风机,达到既散热又节能降噪的目的。在外加电场的驱动下,压电陶瓷片2的逆压电效应带动大型叶片3振荡,这种振荡运动又带动周围空气振荡,如同风扇一样,从而可以对散热管1强迫对流换热。This patent is to use the inverse piezoelectric effect of the piezoelectric
在实际应用中,使用本实施例的压电空冷系统如图3所示。In practical application, the piezoelectric air cooling system using this embodiment is shown in FIG. 3 .
进一步对于空冷冷凝器部分,以600MW直接空冷冷凝器为研究对象,考虑到压电式风扇的固定,将现有的“∧”形布置的冷凝器改为垂直布置。如图4所示,从汽轮机7低压缸排出的乏汽,经由排汽管道9引出主厂房外,通过蒸汽分配管将乏汽引入空冷冷凝器顶部的配汽联箱。直接空冷冷凝器分为若干单元,每个单元又由若干组散热管1组成。采用本实施例后,由于在竖直排列的散热管1侧面布置有若干压电式风扇,给压电陶瓷片2通微弱的电压后,它就会带动叶片3振动,并且能将压电陶瓷片2的小尺度振动转换为叶片3的大尺度共振。这就能取代现有直接空冷系统中的轴流风机,从而实现“低能耗”,“低噪音”的节能性新系统。Further, for the air-cooled condenser part, the 600MW direct air-cooled condenser is taken as the research object, and the existing "∧" shaped condenser is changed to a vertical arrangement in consideration of the fixing of the piezoelectric fan. As shown in Figure 4, the exhaust steam discharged from the low-pressure cylinder of the
在上述技术方案中,根据压电式风扇叶片3特性的相关资料,研究了无环境风速时叶片3到散热管1之间的距离d,各叶片3之间的间距m,叶片3长度l,振动频率f,叶片3的布置形式,这些参数变化时对散热效果的影响。通过模拟得到散热管1壁面法线方向上的温度梯度,并求出对应的表面传热系数。其研究结果如图5至图9所示。In the above-mentioned technical scheme, according to the relevant data of the characteristics of the
从图9中可以看出,叶片3单侧和对称两种不同布置情况下,背风侧和迎风侧表面传热系数的差别。It can be seen from Fig. 9 that the difference in surface heat transfer coefficient between the leeward side and the windward side under two different arrangements of
当叶片3采用单侧布置时,背风侧的表面传热系数很小,仅为迎风侧的1/2左右,图中A为背风侧的表面传热系数,B表示迎风侧的表面传热系数。图中C为对称布置时散热管1壁的表面传热系数,采用对称布置情况下的表面传热系数比单侧布置时迎风侧的小,但只减少了0.17W/(m2·K),这是由于采用对称布置时,两个叶片间相互会有所影响,使散热管1周围的空气扩散受阻,流速下降,从而使换热效果变差。When the
按照相似原理,对流换热的实验数据应当表示成相似准则数之间的函数关系,根据以上模拟结果,可以拟合出散热管1壁面上流体的无量纲温度梯度。由上面的结果可以看出单根管的温度梯度与l/d及Re有关。According to the similarity principle, the experimental data of convective heat transfer should be expressed as a functional relationship between the similarity criterion numbers. According to the above simulation results, the dimensionless temperature gradient of the fluid on the wall surface of
对上述计算结果进行线性回归,可得叶片3振动对散热管1换热影响的无量纲准则关系,其中Nu为努塞尔数,Re为雷诺数:Linear regression is performed on the above calculation results, and the dimensionless criterion relationship of the influence of the vibration of the
利用流体分析软件Fluent模拟不同叶片3参数对空冷散热管1换热效果的影响,对不同工况下数值模拟结果的分析,可以得到以下结论:Using the fluid analysis software Fluent to simulate the influence of
1.叶片3到散热管1之间的距离d会对换热效果产生影响,其取值范围为0.05~0.15米,当距离小于0.1米时,表面传热系数随着距离的增加而增大,距离大于0.1米后,叶片3对散热管1壁面附近的空气扰动作用减少,造成传热性能下降。因此,建议取距离为0.1米为最佳值。1. The distance d between the
2.叶片3的布置间距m对换热性能也会产生影响,其取值范围为0.1~0.3米,总体趋势是表面传热系数随着间距的增加而减小,但减幅有所不同,间距在0.1米到0.2米之间时,下降较平缓;0.2米以后,表面传热系数减小的幅度较大。2. The arrangement distance m of the
3.叶片3长度l对换热性能也会产生影响,其取值范围为0.3~0.7米,随着叶片3长度l的增加,散热管1的换热效果总体上是增加的,但是增幅逐渐减缓,长度小于0.5米时,表面传热系数随长度增加而增大的速度较快,长度大于0.5米后,长度对换热性能的影响基本可以忽略不计。考虑到叶片3的固定,建议取0.5米。3. The length l of the
4.增大叶片3振动频率f也能改善散热,但在一定范围内,对散热的影响并不大,显示出了与叶片3长度相似的影响。考虑到我国的工频是50Hz,建议取50Hz。为了将噪音降低到最低限度,可将频率取在人耳所能感知的范围之外。4. Increasing the vibration frequency f of the
5.叶片3的布置形式影响到散热管1的换热性能,叶片3布置在散热管1单侧时,迎风侧的表面传热系数大概是背风侧的两倍左右;叶片3对称布置在散热管1两侧时,两侧的表面传热系数基本相同,与单侧布置时迎风侧的表面传热系数相比有所下降,但降低的并不多。因此,建议采用叶片3两侧对称布置的形式。5. The layout of the
综上所述,与传统的空冷冷凝器相比,本发明空冷冷凝器具有换热能力强、耗能低、无噪音等优点,并将以其优异的换热性能在空冷冷凝器等换热环境得到广泛应用。In summary, compared with the traditional air-cooled condenser, the air-cooled condenser of the present invention has the advantages of strong heat transfer capacity, low energy consumption, no noise, etc. environment is widely used.
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