共查询到18条相似文献,搜索用时 453 毫秒
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建立了一种有关切向流对小孔声阻抗影响的小扰动势流模型,其要点是使用法向质点速度连续而非广为采用的质点位移连续边界条件来匹配小孔剪切层两侧的声场,并在小孔前缘施加Kutta条件以反映切向流效应的机理———锐缘处的声涡转化。模型中还包含了实际应用中经常遇到的小孔形状和穿孔板厚度两个重要因素。理论预测的声阻和声抗与实验结果良好吻合。 相似文献
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为了发展大涵道比发动机噪声传播途径控制的降噪技术,基于数值仿真与优化算法,以某型大涵道比风扇/增压级试验
件为应用对象,开展进口单自由度声衬设计。在声衬设计过程中,采用非线性谐波法对省略内涵增压级的简化结构进行模拟,并
在光壁及声阻为0~5、声抗为-5~5条件下,以此作为声源开展基于有限元方法的声传播模拟。在固定声衬穿孔板厚度及穿孔直径
的情况下,采用Guess声阻抗模型,将声阻抗-降噪量关系映射到声衬几何参数-降噪量关系,获得声衬几何参数-降噪量图谱,筛
选出最佳声衬几何(参数),同时采用模拟退火优化算法获得最大降噪效果的声衬几何参数,并与遍历算法结果进行对比,开展不同状
态条件下的降噪效果评估。结果表明:该声衬在风扇0.8转速状态及起飞状态下对1BPF的风扇噪声具有良好的降噪效果。 相似文献
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研究了一种带可调背腔的多孔径穿孔板声阻尼器的吸声特性,并通过声学模型预测了穿孔板的吸声特性。实验研究了偏流穿孔板对液雾燃烧器的燃烧室、气室内波动的动态压力及热释放率的控制效果。多孔径穿孔板存在两种孔径:小孔半径均为1.0 mm,大孔半径分别为1.5、2.0、2.5、3.0 mm。发现孔径差异过大的穿孔板消声性能不佳。但是大小孔径相近的穿孔板对腔室内的热声振荡有明显衰减效果。安装穿孔板后,燃烧室脉动压力下降59%~84%,放热波动下降47%~87%,同时火焰形态变得稳定。 相似文献
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偏流板对发动机进口温升影响研究 总被引:1,自引:0,他引:1
为研究偏流板升起条件下发动机进口温升的变化,采用计算流体动力学的方法,计算了不同的发动机推力状态、偏流板板位角、偏流板与发动机距离对流场和发动机进口温升的影响。结果表明:在偏流板升起时,随着发动机推力状态的升高,发动机进口温升逐渐增大;随着板位角的增大,高温燃气沿甲板向发动机进口方向扩散范围越大,进口温升逐渐增大;在相同发动机推力状态和板位角时,增加偏流板与发动机距离可显著减小发动机进口温升。 相似文献
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通过实验方法研究了热声不稳定性极其被动控制方法。搭建了水平放置的Rijke管热声不稳定性实验装置,采用电加热的热丝作为热源。实验中发现加热功率及加热丝前后空气的温度比对热声不稳定性的发声强度有着一定的影响。实验中尝试了采用背腔和穿孔板结构的声衬对热声不稳定性进行控制。其中背腔中可以通入偏流空气,且偏流空气的流量、温度均可以调节。实验发现:背腔中通入偏流空气可以增强对不稳定性的抑制效果,且随偏流速的增加,控制效果变好。此外,发现提高偏流空气的温度对提高声衬对热声不稳定性的控制效果作用不明显。 相似文献
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舰载机在加力起飞时通过舰面安装的偏流板将高温尾喷流引向空中排出,避免了高温尾喷流损伤舰面工作人员和舰载设备,但一部分高温尾喷流与偏流板碰撞后的回流受发动机抽吸作用的影响,容易被进气道吸入,导致发动机推力降低,严重时诱发发动机喘振,危害舰载机的使用安全。为了获得高温尾喷流与偏流板碰撞后的回流场流动机理以及参数影响规律,采用数值仿真分析方法开展了研究。首先,通过公开的试验数据验证了仿真分析方法的准确性;然后,完成了舰面环境下某型舰载机双发尾喷流冲击偏流板后的流动机理和温度场特征分析,获得了高温气体被进气道吸入的动态流动特性和进气道出口的温升率;最后,通过研究发动机转速不对称、来流风速、尾喷口到偏流板距离等参数对进气道出口温度畸变强度的影响规律,获得了尾喷口到偏流板的距离对回流场整体强度与分布起决定作用,以及进气口的位置影响进气道抽吸流场与回流场的耦合特性这一结论。 相似文献
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偏流板回流对舰载机进气道温升影响分析 总被引:3,自引:0,他引:3
为了探究舰载机起飞时发动机尾喷流撞击偏流板( Jet Blast Deflector,JBD)后反射回流对进气道温升的影响,以模型机和喷气偏流板为研究对象,通过求解三维雷诺平均纳维-斯托克斯方程和Menter SST湍流模型方程,对舰载机准备起飞时的飞机内、外流场进行了数值模拟。利用线积分卷积方法对流场进行了可视化显示,分别研究了JBD不同倾角以及不同环境风速情况下,喷流回流对进气道温升的影响。计算结果表明:环境风速保持不变,在JBD倾角由30°逐步增大到60°的过程中,进气道出口截面面平均温升(ΔTav )总体呈增大趋势,当倾角由45°变为50°,进气道出口截面面平均温升陡增;对于特定的JBD倾角,在环境风速逐步增大过程中,存在一个临界风速,当风速小于临界风速时,进气道出口截面ΔTav随风速增加而增大。当风速大于临界风速时,进气道出口截面ΔTav随风速增加而显著降低。计算结果对于偏流板布局选择具有一定的指导意义。 相似文献
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In order to address the current aircraft noise problem, the knowledge of impedance of acoustic liners subjected to high-intensity sound and grazing flow is of crucial importance to the design of high-efficiency acoustic nacelles. To this end, the present study is twofold. Firstly, the StraightForward impedance eduction Method (SFM) is evaluated by the strategy that the impedance of a liner specimen is firstly experimentally educed on a flow duct using the SFM, and then its accuracy is checked by comparing the numerical prediction with the measured wall sound pressure of the flow duct. Secondly, the effects of grazing flow and high-intensity sound on the impedance behavior of two single-layer liners are investigated based on comparisons between educed impedance and predictions by three impedance models. The performance of the SFM is validated by showing that the educed impedance leads to excellent agreement between the simulation and the measured wall sound pressure for different grazing flow Mach numbers and Sound Pressure Levels (SPLs) and over a frequency range from 3000?Hz down to 500?Hz. The grazing flow effect generally has the tendency that the acoustic resistance exhibits a slight decrease before it increases linearly with an increase in Mach, predicted successfully by the sound-vortex interaction theoretical model and the Kooi semi-empirical impedance model. However, the Goodrich semi-empirical impedance model gives only a simple linear relation of acoustic resistance starting from Mach zero. Additionally, when the SPL increases from 110 to 140?dB in the present investigation, the acoustic resistance exhibits a significant increase at all frequencies in the absence of flow; however, the resistance decreases slightly under a grazing flow of Mach 0.117. It indicates that the SPL effect can be greatly inhibited when flow is present, and the grazing flow effect can be reduced partly as well at a relatively high SPL. 相似文献
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使用声学流管实验台对一件双自由度(DDOF)声衬和一件单自由度(SDOF)声衬的声学特性进行对比测试。在最大0.26Ma切向流速和管道的截止频率之下,采用直接提取法SFM测得声衬的无量纲声阻抗,同时使用双传声器分解驻波法计算声衬安装段管道的传声损失(TL)和吸声系数等,基于声能量理论的传声损失可直观地展示两件被测声衬的吸声性能差异。结果表明在流管声学实验台上,相较于单自由度声衬,双自由度声衬能够有效拓宽声衬的吸声频带,同时共振频率处的传声损失不如单自由度声衬,切向流也会明显改变声衬的共振频率、弱化吸声能力。基于声能量的传声损失和吸声系数也为无等效阻抗的非均匀结构声衬提供了一种声学性能评估方法。 相似文献
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通过采用外部声激励的方式,在低速轴流压气机内研究非定常尾流撞击效应对压气机流场结构以及时均气动性能的影响。主要包括:低速轴流压气机实验台的流场调试;流场的稳态、动态测量;实验数据的处理和分析。实验结果表明:当发生尾流撞击耦合效应时,压气机内部流动的时空结构以及时均气动性能均得到较大提高。 相似文献
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This paper describes a new experimental approach to acoustic liner characterization in the presence of a grazing flow. The traditional methods of measurement use microphones to determine liner impedance. The in situ method in particular requires the simultaneous use of two microphones. The first is mounted flush with the surface of the liner grazed by the flow and the second is flush-mounted to the rear face of the liner. However, this method is invasive and assumes the reaction of the liner to be independent of the incidence of the waves (locally-reacting liner). The approach suggested here is radically different since Laser Doppler Velocimetry (LDV) is used to measure the acoustic perturbation of velocity, or acoustic velocity. This latter allows us to determine the acoustic displacement, which is the key parameter in Galbrun's linear theory for assessing the perturbation of pressure and the field of active intensity. The wall impedance and the propagation paths of acoustic energy in the presence of the liner may be deduced without any assumption and non-invasively. This approach was applied for characterizing a resistive liner in a test bench specially designed for aeroacoustic measurements, with a 2D LDV system. The flow was turbulent and the measured nominal Mach number was 0.13. The impedance and field of active intensity were then obtained. A comparison was carried out between the new approach and the in situ method using microphones. According to previous theoretical works in the literature and the presented test results, one has to be cautious about the definition of the impedance when performing in-flow acoustic measurements. 相似文献