共查询到17条相似文献,搜索用时 703 毫秒
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针对热声发动机中复杂的起振、消振行为,在自行研制的"驻波型热声发动机试验平台"上,开展了工质类型、加热功率、充气压力等参数对热声发动机起振、消振行为的影响规律研究.试验结果表明:当采用纯氦气和90%氦气+10%氩气的混合气体时,系统存在一最佳的充气压力值,使起振温度和消振温度达到最低;而其余工质,其起振温度与消振温度均随着充气压力增加而逐渐提高;与此同时,由于加热功率对板叠热端温度影响较小,故采用板叠热端温度作为行为特性参数更为合理. 相似文献
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针对热声发动机起振过程中复杂的温度变化,在自行研制的"驻波型热声发动机试验平台"上,开展了在不同的工质类型、充气压力等试验工况下,热声发动机起振过程的轴向温度分布规律和变化特征的试验研究,试验结果表明:对于氮气、氩气而言,其系统温度动态特性规律基本一致,且热声核温度梯度和热声板叠温度梯度存在较明显的差别;而对于氦气,其系统温度动态特性不同于前两类气体,且热声核的温度梯度和热声板叠温度梯度的差别十分微弱,可见,不同的工质类型将直接影响到发动机起振过程系统温度的动态变化特性. 相似文献
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采用气液耦合振动是降低热声发动机谐振频率和提升其压力振幅的一种有效途径。为了研究液体工质对于气液热声发动机性能的影响,本文针对水、室温离子液体[EMIM][BF4]、20%氯化钾溶液、40%和50%甲酸钾溶液五种液体工质进行了实验研究和分析。实验数据显示,在相同加热功率下,采用50%甲酸钾溶液时系统谐振频率最低,而水工质对应的谐振频率最高;40%甲酸钾溶液的压力振幅最大,而采用离子液体[EMIM][BF4]时系统压力振幅最小。研究结果表明:采用密度较大的液体工质可获得较低的谐振频率,而密度大、黏度小的液体工质则有利于获得更大的压力振幅。 相似文献
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《工程热物理学报》2010,(6)
设计搭建了太阳能热声发动机实验系统,它由双轴全自动跟踪菲涅尔透镜聚焦型集热器和小型化驻波热声发动机两大组件构成。分别对充注不同压力N_2、He、Ar三种工质的太阳能热声发动机的起振温度、起振时热声核温度分布、压力振幅进行了实验研究。结果表明,氮气、氦气和氩气在相同充气压力下,He起振温度最高,N_2起振温度最低;N_2在充气压力1.0 MPa时达到最低起振温度394.8℃,且其压力振幅对充气压力变化不敏感;Ar在充气压力1.0 MPa时达到最低起振温度418.2℃,且其压力振幅随着充气压力的升高而逐渐增加。实验结果为优化太阳能热声发动机系统的热力性能提供了实验依据。 相似文献
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古鑫何雅玲沈超张东伟李玉光 《工程热物理学报》2014,(6):1040-1044
设计搭建了一台由双轴跟踪菲涅耳透镜集热器和驻波发动机组成的太阳能热声发动机,并在此基础上研究了不同工质配比、板叠厚度和谐振管长度对起消振温度和压力振幅的影响。实验结果表明,当氦气摩尔比为0.25~0.50时,混合气体有更低的起消振温度和更大的压力振幅。当板叠厚度由0.45 mm减至0.15mm时,起振和消振温度降低,压力振幅上升。随着谐振管长度的增加,起消振温度降低,压力振幅提高,当谐振管管长2.1 m时分别获得297℃和176℃的最低起振和消振温度,以及69.1 kPa的最大压力振幅。 相似文献
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磁致伸缩换能器辐射板形状对声场分布的影响 总被引:1,自引:0,他引:1
磁致伸缩换能器可作为热声制冷机的声源装置,辐射板的形状直接影响声压输出效率,从而影响制冷效果。为提高换能器工作效率、减小换能器体积,辐射板需在Terfenol-D棒的激励下产生大振幅、高频率的活塞振型。针对这一问题,应用ATILA软件分析了磁致伸缩换能器辐射板形状对谐振腔振动幅频特性的影响以及对谐振腔内声场分布的影响。结果表明:相同激励条件下,凹球面辐射板出现活塞振型时振幅最大,对应谐振腔中声压幅值最高;谐振腔端面形状为凹球面时,具有聚焦声压幅值的作用;端面形状为凹发射端-凸反射端组合的谐振腔内声压幅值最高。以上结论为合理设计辐射板、谐振腔两端面组合形状提供了参考。 相似文献
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The influence of the resonator shape on nonlinear acoustic field in a thermoacoustic engine is studied.The resonator of themoacoustic engine is boundary driving by a piston at one end,and the other end of it is rigid closed.A one-dimensional wave equation that accounts for gas dynamic nonlinearities and viscous dissipation in the resonator is established based on the governing equations of viscous hydromechanics.The nonlinear wave equation is solved using approximate Galerkin method.The nonlinear acoustic field in four different types of shaped resonators including hyperbolical,exponential,conical and sinusoidal are obtained and compared with that of a cylindrical resonator.It is found that the amplitude and waveform of the pressure are strongly affected by the resonator shape,the driving amplitude and the oscillation frequency of the piston.Waveform distortion,resonance frequency shift and hysteresis are observed,when the piston oscillation amplitude is large enough.The advantages of shaped resonator for thermoacoustic engine lie in inhibition of higher order harmonics and improvement of pressure ratio,etc. 相似文献
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Experimental studies on perturbed acoustic resonant spectroscopy by a small rock sample in a cylindrical cavity 总被引:5,自引:2,他引:3
CHEN Dehua WANG Xiuming CONG Jiansheng XU Delong SONG Yanjie MA Shuilong 《中国科学G辑(英文版)》2006,49(6):683-701
A measurement system for acoustic resonant spectroscopy (ARS) is established, and the effects of resonant cavity geometry,
inner perturbation samples and environmental temperature on the ARS are investigated. The ARSs of the small samples with various
sizes and acoustic properties are measured. The results show that at the normal pressure, the resonant frequency decreases
gradually with the increase of liquid temperature in the cylindrical cavity, while the resonant amplitude increases. At certain
pressure and temperature, both the resonant frequency and the amplitude decrease greatly when there exist air bubbles inside
the cavity fluid. The ARS is apparently affected by the sample porosity and the sample location in the resonant cavity. At
the middle of the cavity, the resonant frequencies reach their maximum values for all of the measurement samples. The resonant
frequencies of the porous rock samples are smaller than those of the compacted samples if other acoustic parameters are the
same. As the sample is moved from the top to the middle of the cavity along its axis, the resonant amplitude increases gradually
for the compacted rocks while decreases for the unconsolidated rocks. Furthermore, the resonant amplitude increases firstly
and then decreases if the porosity of the rock sample is relatively small. In addition, through the comparisons between the
experimental and theoretical results, it is found that the effects of the acoustic parameters and sizes of the samples and
the size of the cylindrical cavity on the laboratory results agree well with the theoretical ones qualitatively. These results
may provide basic reference for the experiment study of rock acoustic properties in a low frequency using ARS. 相似文献