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1.
在热声发动机系统中,谐振管用来调节系统的超振频率.通常的四分之一波长谐振管由一段谐振管后面连接一个比较大的气体容积构成,与二分之一波长谐振管相比,在相同的起振频率下前者可以有相对短的管长.锥形谐振管除了调节频率外,还可以提高热声发动机输出压力波的压比.本文通过数值计算软件Fluent6.0中的K-ε湍流模型模拟了不同长度、不同的进出口直径的一系列锥形谐振管,得出了近似四分之一波长锥形谐振管的共振频率与其长度、锥度之间的关系,并初步与实验进行了对照.  相似文献   

2.
本文基于包含流动和传热两个方面的电路类比理论,针对一具有环路结构的气液相变热声发动机系统进行了模拟计算和分析。重点讨论了排出器、动力活塞、反馈管以及负载液柱的直径和长度对于系统谐振频率和换热器驱动温度梯度的影响。结果显示,该气液相变热声发动机的谐振频率较低(小于1 Hz),排出器和动力活塞的直径,以及反馈管的直径和长度对于谐振频率的影响较大;气液相变热声发动机所需驱动温度梯度比通常气体工质热声发动机小一到两个数量级,各主要部件的直径对气液相变热声发动机所需驱动温度梯度的影响比长度对其影响更为显著。  相似文献   

3.
谐振管是热声热机的主要部件之一,减小声功在谐振管中的耗散对改善热声热机输出特性具有积极意义。由于近临界区流体的热物性具有特殊性,用其作为工质时将会对谐振管内的声功损耗产生重要影响。本文对声功在以近临界区CO_2为工质的谐振管中的损耗情况进行了计算和分析。结果显示,在本文的计算条件下,相较于压力较低的CO_2,采用近临界区CO_2作为工质可降低谐振管内的声功损耗,并在工作压力略低于临界压力时,谐振管内的声功损耗可达到最小值.此外,在保持谐振频率不变的情况下,采用近临界区CO_2作为工质可一定程度上缩短谐振管的长度。  相似文献   

4.
传统的行波热声发动机具有可靠性好、工质环保、潜在效率高等优点,但系统中存在一根体积较大的谐振管,降低了其功率密度及应用价值。本文设计并搭建了一台新型的声学共振型行波热声发动机,将三个相同的热声发动机核心单元连成环路,中间采用细长谐振管连接。实验中,发动机在100℃以下起振,频率约63 Hz,各压力下得到的最高压比均接近1.3,达到了传统行波热声发动机的最高压比。实验表明,新型的声学共振型行波热声发动机不仅具有传统行波热声发动机的优点,而且结构更加紧凑,具有更好的应用价值。  相似文献   

5.
本文根据经典热声学理论,对声学双作用型行波热声发动机系统进行了全面的损失分析。系统产生的损失可以分为内部不可逆损失与外部不可逆损失,其中内部损失可区分为:轴向漏热损失,流体黏性损失,不可逆传热损失与流动传热耦合损失。本文对一台效率为55.7%的声学双作用型行波热声发动机进行了具体的媚损失分析,结果显示,回热器与谐振管是产生损失最多的部件。谐振管中的损失主要是流动损失,而回热器中的流动损失则相对较少。  相似文献   

6.
回热器中填充了玻璃丝绵,在声驱动的热声谐振管中发生共振,通过测量谐振频率,分析热声谐振管的频率特性,辨识谐振管的品质因数,其测量结果能与理论计算值较好的吻合。实验证实,品质因数是评价热声谐振管工作性能的重要参数。  相似文献   

7.
优化设计并研制了一小冷量液氮温区高频热驱动脉冲管制冷机,系统轴向长度仅为1.2 m.针对之前系统热效率较低问题,在数值计算的指导下,对高频驻波热声发动机的板叠流道尺寸和热腔进行了优化,并对声压放大器进行了调整.采用4.0 MPa氦气为工质,在发动机端加入750 W加热量获得了68.3 K的最低制冷温度,这是目前国际上报道的高频热驱动脉冲管制冷机的最低制冷温度.加入500 W加热量时,制冷机获得了76.9 K的无负荷最低制冷温度,在80 K时有0.2 W的制冷量.  相似文献   

8.
时均流激声发动机利用流体诱导声振荡效应把自然界的风和管道气体的动能转化为声场能,可驱动热声制冷机制冷或驱动发电机和换能器发电,为风能利用提供了新思路。在国内首次搭建了正十字型时均流激声发动机实验台,以一台高压风机提供的气流模拟自然风,获得了稳定的驻波声场。在此基础上,揭示了时均流速、平均压力、斯特劳哈尔数等对时均流诱导声振荡的影响。在平均压力为106.19 kPa、时均流速为50.52 m/s、谐振管长度为0.96 m的条件下,该正十字型时均流激声发动机谐振管内的压力振幅达6.20 kPa,约为平均压力的5.80%,为时均流激声发动机驱动发电装置和热声制冷研究奠定了实验基础。  相似文献   

9.
汪拓  吴锋  李端勇  陈浩  林杰 《物理学报》2015,64(4):44301-044301
热声发动机的起振过程是一个产生并维持自激振荡的过程, 研究热声自激振荡机理有助于进一步了解热声效应的实质. 根据热声网络理论, 建立了驻波热声发动机的整机网络. 将热声网络比拟成电网络, 利用厄米特式计算了输入热声网络的视在功流, 功流平衡对应自激, 在角频率虚部为零的情况下计算了热声发动机的阈值温度和运行频率. 结果表明, 计算值与实验值符合得较好, 充气压力与阈值温度和运行频率的耦合关系大致相同. 所得结论有助于进一步探究热声效应机理以及热声发动机系统的优化设计.  相似文献   

10.
时均流诱导的声振荡可以为热声制冷提供驱动源或驱动发电机和换能器发电,为风能利用提供了新思路,是热声领域的最新研究方向之一。本文基于计算流体动力学(CFD)方法,建立了正十字型时均流激声发动机的三维数学模型,采用大涡模拟湍流模型计算。计算结果验证了时均流诱导声振荡效应,揭示出谐振管内声场分布和谐振管内部压力与开口处涡的关系,为后续的实验研究奠定了理论基础。  相似文献   

11.
韦克  刘旭  陈宇 《应用声学》2008,27(2):113-117
把改进的12-Bit格子气模型用于复杂边界的热声发动机的模拟研究,成功模拟了带共振腔的驻波管中热声振荡演化过程。对热声板叠的长度、热声板叠在共振管中的位置以及共振腔的几何大小对热声振荡振幅的影响进行了数值计算。计算结果显示,当共振腔与细管的宽度比为2.2,板叠位置相对于细管长为0.34时,驻波管中热声振荡振幅达到最大。共振腔尺寸的研究,对于热声发动机性能的的优化设计有指导意义。  相似文献   

12.
Acoustic streaming in closed thermoacoustic devices.   总被引:2,自引:0,他引:2  
A derivation of acoustic streaming in a steady-state thermoacoustic device is presented in the case of zero second-order time-averaged mass flux across the resonator section (nonlooped device). This yields analytical expressions for the time-independent second-order velocity, pressure gradient, and time-averaged mass flux in a fluid supporting a temperature gradient and confined between widely to closely separated solid boundaries, both in the parallel plate and in the cylindrical tube geometries (two-dimensional problem). From this, streaming can be evaluated in a thermoacoustic stack, regenerator, pulse tube, main resonator of a thermoacoustic device, or in any closed tube that supports a mean temperature gradient, providing only that the acoustic pressure, the longitudinal derivative of the pressure, and the mean temperature variation are known.  相似文献   

13.
Linear thermoacoustic theory is currently well accepted for simulating thermoacoustic systems, and correction is used to reduce the discrepancy between calculations and experimental results for turbulent flow. In order to calculate passive tube systems and make linear thermoacoustic theory coincide closely with experiments, a passive network model based on fluid network theory is derived. An amendment method is proposed to further correct for turbulence by amending thermal and viscous penetration depths when the ratio of the tube radius to the viscous penetration depth R/δv is large. The experiments have been done to verify the model in the acoustic amplifier, Helmholtz resonator, and inertance tube. In addition, the mechanisms of such tubes are further analyzed based on the model.  相似文献   

14.
Thermoacoustic engines convert heat energy into high amplitude sound waves, which is used to drive thermoacoustic refrigerator or pulse tube cryocoolers by replacing the mechanical pistons such as compressors. The increasing interest in thermoacoustic technology is of its potentiality of no exotic materials, low cost and high reliability compared to vapor compression refrigeration systems. The experimental setup has been built based on the linear thermoacoustic model and some simple design parameters. The engines produce acoustic energy at the temperature difference of 325–450 K imposed along the stack of the system. This work illustrates the influence of stack parameters such as plate thickness (PT) and plate spacing (PS) with resonator length on the performance of thermoacoustic engine, which are measured in terms of onset temperature difference, resonance frequency and pressure amplitude using air as a working fluid. The results obtained from the experiments are in good agreement with the theoretical results from DeltaEc.  相似文献   

15.
热声制冷机主要由声驱动器、共振管、板叠、高低温端换热器、声容等部件组成。它具有运动部件少、运行可靠、振动小和寿命长等优点 ,在军事、航天、微电子、低温物理等领域有着十分诱人的应用前景。文中运用经典线性热声理论对热声制冷机各个组成部件设计进行了介绍 ,在此基础上设计了一台扬声器驱动热声制冷机 ,并用专业计算软件进行了数值模拟验证 ,为热声制冷机进一步优化与发展提供了一个解决方案。  相似文献   

16.
A low-frequency open-air thermoacoustic engine in a Helmholtz resonator has been constructed. Tests indicate that the system resonates in the Helmholtz mode for modest thermoacoustic stack temperature differences using stacks of varying type and pore size located within the neck of the Helmholtz resonator. The maximum acoustic pressure radiated from the open end of the resonator corresponds to 81 dB-SPL ref 20 μPa at a stack temperature difference of 185 K and an input electric power of 276 W. The system is well characterized by a numerical model of a representative stack.  相似文献   

17.
Thermoacoustic oscillation is a significant problem in ducted domestic heating systems fitted with fully premixing burners as well as in combustion systems of industrial scale. This paper reports experiments using a burner closely representative of practical designs in which high-intensity free-field sound has been used to simulate the feedback which may be excited naturally in installations with different acoustic properties. This experimental approach facilitates study of the non-linear response of the burner/flame sub-system to feedback of different frequencies and direct measurement of the acoustic impedance of the burner under operational conditions. A function proportional to the Rayleigh integral has been evaluated directly from the experimental results. It is found that the head of this type of burner divides the typical installation into a quarter-wave tube and a Helmholtz resonator which must couple unstably for thermoacoustic oscillations to be autoexciting. It is further found that there is a strong interaction between the acoustic field and the mean flow which modifies significantly the behaviour of the burner as a Helmholtz resonator and thus the stability of the whole system.  相似文献   

18.
研究了谐振管一端受活塞声源激励,另一端刚性封闭条件下,管道形状对热声发动机谐振管内部非线性声场的影响。基于流体力学基本方程建立了渐变截面谐振管内一维非线性声场的模型,考虑了黏性耗散及非线性效应的影响。利用伽辽金法数值求解了该模型的速度势方程,分析了谐振管形状、活塞振动速度及激励频率对管内声场的影响。将双曲形、指数形、锥形、正弦形等四种变截面谐振管内的非线性声场与圆柱形直管的情况进行了比较。结果反映了谐振管内声场的压力波动受活塞振动速度及谐振管形状的影响;显示了当活塞振动幅度较大时,谐振管内出现的波形畸变、频率曲线偏移、共振频率滞后等非线性现象;揭示了变截面谐振管在抑制管内的高阶谐波及提高压比等方面的优越性。   相似文献   

19.
针对本实验室一台声驱动热声系统,采用传递函数法研究声驱动系统中回热器的特征阻抗和传播常数.通过调节谐振管长度,改变回热器表面的阻抗,从理论上分析了回热器网络传输方程中的声传播常数、特征阻抗与系统网络元件中的阻抗、导纳和流的关系.并且进一步讨论有无换热器以及不同的加热功率对回热器网络参数的影响.结论有利于进一步量化回热器的网络参数.  相似文献   

20.
Luo EC  Ling H  Dai W  Yu GY 《Ultrasonics》2006,44(Z1):e1507-e1509
In this paper, an experimental study of the effect of the resonator shape on the performance of a traveling-wave thermoacoustic engine is presented. Two different resonators were tested in the thermoacoustic-Stirling heat. One resonator is an iso-diameter one, and the other is a tapered one. To have a reasonable comparison reference, we keep the same traveling-wave loop, the same resonant frequency and the same operating pressure. The experiment showed that the resonator shape has significant influence on the global performance of the thermoacoustic-Stirling heat engine. The tapered resonator gives much better performance than the iso-diameter resonator. The tapered resonator system achieved a maximum pressure ratio of about 1.3, a maximum net acoustical power output of about 450 W and a highest thermoacoustic efficiency of about 25%.  相似文献   

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