共查询到17条相似文献,搜索用时 169 毫秒
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为探究预旋结构如何影响盖盘系统内的流动特性,对不同预旋角度和进气位置的带盖盘预旋系统进行实验研究,得到了高转速下静盘表面静压和中心面总压的分布、中心面旋流系数、预旋孔排气系数以及腔内流阻系数。结果表明:预旋角度和进气位置分别影响腔内压力分布大小和分布趋势。随预旋比增加中心面旋流系数整体增加,转静腔内旋流系数与无量纲半径的-2次幂存在线性关系。预旋孔排气系数随预旋孔进出口压比的增加而增加。流阻系数随湍流参数增大而上升,随旋转雷诺数的增加而减小。 相似文献
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高旋转雷诺数下预旋进气转-静盘腔流动换热特性 总被引:5,自引:3,他引:2
运用RNG k-ε湍流模型对高旋转雷诺数和预旋进口速度下,静盘外缘预旋进气、转盘外缘轴向出流模型的流动和换热过程进行了三维数值模拟,主要研究了冷气流量Cw、旋转雷诺数R ee等参数对转盘对流换热系数和出流口温度分布的影响,并与垂直进气方式进行了对比。研究表明:预旋进气方式与垂直进气相比可降低涡轮叶片冷气入口总温;冷气流量增大以及旋转雷诺数增大均使得转盘平均换热增强;涡轮叶片入口温度随冷气流量增大而降低,随着旋转雷诺数的增大先升高后降低。 相似文献
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有去旋进气共转盘腔内流动换热数值模拟 总被引:2,自引:1,他引:1
对左边转盘高位带去旋孔且附有内隔片的共转盘腔内的流动和换热进行了数值模拟.揭示了去旋角、旋转雷诺数、去旋喷嘴进气无量纲流量系数等参数对共转盘腔内的流动结构、压力损失和换热效果的影响.结果表明:盘腔内的总压降随无量纲流量系数的增加呈"S"形变化趋势;旋转雷诺数和冷气无量纲流量系数的增大都能增强转盘表面的换热效果;与预旋转静盘腔相比,去旋进气共转盘腔能使出口气流温度更低,冷却效果更好. 相似文献
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带盖板的预旋系统温降和压力损失数值研究 总被引:13,自引:5,他引:8
为了更大限度地挖掘预旋系统的温降潜力,对有盖板的预旋进气转-静盘腔内的气动热力问题进行了数值模拟,研究了旋转雷诺数、无量纲流量和旋转比对系统温降和压力损失特性的影响,结合盘腔内的流动特征分析了预旋温降和压力损失机理.计算表明绝热条件下的预旋温降主要受动静坐标系转换引起的动降温、离心升温,以及摩阻做功与黏性耗散等不可逆因素三方面影响,其中动降温取决于气流速度和相对速度,这些因素综合决定了系统温降随旋转雷诺数、无量纲流量和旋转比的变化规律.系统压降主要受气动损失、离心升压和坐标系转换引起的动压变化三方面影响.数据显示旋转比是无量纲温降和压力损失系数的主要影响因素.还讨论了预旋孔和接受孔流量系数随流量、转速和旋转比的变化规律. 相似文献
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分别对预旋角度为20°的直孔和扩口孔型喷嘴进行了数值模拟和实验测量.计算模型包括仅有进气腔、预旋孔和出气腔的单独模型和在此基础上增加了旋转部分的系统模型;研究内容包括速度场、出气速度、出气角度、流量系数、预旋效率和温降,并对单独模型的孔流量系数进行了实验测量.结果表明流量系数的计算结果与实验结果符合良好,扩口孔的流量系数、预旋效率和温降都比直孔显著增大20%以上.数据还显示由单独模型计算得到的流量系数和预旋效率与由系统模型得到的结果比较接近,根据单独模型的预旋效率而推算出的温降可在一定程度上间接反映预旋系统的温降特性. 相似文献
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带盖板预旋系统的流动实验 总被引:7,自引:4,他引:3
通过低转速的模拟实验对涡轮盘腔的带盖板预旋系统的流动特性进行了研究。在不同的紊流参数(0.5〈λT〈0.96)和旋转比(1.03〈βp〈1.9)下测量了预旋腔和盖板腔内的压力与速度分布,得到了两个腔内的旋转比变化情况,并分析了旋转雷诺数和进出口压比对预旋喷嘴流量系数的影响。实验结果表明:在两个腔内离心升压效应明显,预旋喷嘴出口气流对预旋腔内的气流压力和速度的影响要远大于接收孔出口气流对盖板腔的影响,压比和旋转雷诺数对喷嘴流量系数有较小的影响。 相似文献
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1.5级涡轮实验台前腔燃气入侵实验 总被引:3,自引:1,他引:2
在1.5级涡轮实验台上,针对不同转速和不同封严质量流量,分别采用稳态压力测量、瞬态压力测量和二氧化碳体积分数法对燃气入侵现象进行了实验研究,以确定不同工况下主流的动静叶相互作用对燃气入侵的影响以及入侵到盘腔的燃气在腔内与冷气的掺混过程.结果表明:静叶后的时均压力在周向有明显的周期分布,部分区域封严环外的压力高于腔内压力,且随着封严质量流量增加,这一区域逐渐缩小;动叶扫掠带来同频率的压力波动,对于燃气入侵的发生有着重要的影响;通过二氧化碳体积分数实验获得了最小封严质量流量,并得到在封严质量流量不足情况下燃气沿着静盘侧入侵盘腔的结果. 相似文献
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An experimental investigation into pre-swirl effectiveness and receiver hole discharge coefficient characteristics for a high radius injection pre-swirl cooling systems was carried out on a physically representative experimental rig with a 450 mm diameter rotor.The receiver holes and pre-swirl nozzle were located at a radius of 181 mm and 180 mm respectively.The experimental work was mainly conducted at 5 000~12 000 r/min,4 bar absolute pressure and 1.132 kg/s air supply.The maximum air supply temperature was 190 ℃.Pressure and temperature distributions in the pre-swirl system were examined with an emphasis on the velocity effectiveness of the pre-swirl system as a whole and on the discharge coefficients of the rotating 'receiver holes' in the rotor.The results showed that the velocity effectiveness increased with increasing swirl ratio resulting in reduced blade cooling flow temperature.Different seal flow configurations caused very different effectiveness at different speeds,but outflow through the inner and outer seals always gave the highest effectiveness compared other configurations.Increasing the seal flow rate reduced the effectiveness.For the coefficient of discharge,except for the low speed range,it increased with increase in swirl ratio for most speeds. 相似文献
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Experiments were conducted on a typical rotor-stator system where air entered through an annular slot at low radius and flowed out of the cavity axially through a rim seal between the rotor and the stator. For the seal in this rotor-stator system, the stationary shroud overlapped the rotating one. Pressure distributions at the stator surface and flow resistance coefficients of the rotor-stator cavity with a maximum gap of 67mm were measured under different dimensionless mass flow rates from 1.32×104 to 4.87×104 with a large range of rotational Reynolds numbers from 0.418×106 to 2.484×106. The results show that pressure on the stator surface decreases with the increase of rotational Reynolds number when the dimensionless mass flow rate is below 1.3×104; when the dimensionless mass flow rate is above 3.034×104, the trend reverses. This is the so-called "pressure inversion effect". However, dimensionless pressure does not show the same changes when rotational dynamic pressure is chosen as the denominator. The resistance coefficient of the rotor-stator cavity is determined by the dimensionless mass flow rate and rotational Reynolds number; for practical application, the resistance coefficient can also be estimated by the turbulent flow parameter in the range of turbulent parameter from 0.1 to 1.6. 相似文献