共查询到19条相似文献,搜索用时 93 毫秒
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通过改进等截面驻波管实验系统,在1阶峰值共振频率激励下获得了182.1 dB大振幅驻波场,并对1~5阶峰值共振频率激励下的大振幅驻波场谐波饱和情况以及波形畸变进行了实验研究。研究发现,尽管1阶峰值共振频率激励下声压级已达到182.1 dB,但波形畸变最小,谐波并未表现出饱和现象,而3阶峰值共振频率激励下的大振幅驻波场表现出了饱和趋势。对谷值共振频率激励下获得的大振幅驻波场进行对比实验研究,发现谷值共振频率激励下,1阶谷值共振频率所获得的驻波场声压级最大,但波形畸变也最大。在相同声源驱动电压下,1阶峰值共振频率激励下获得的驻波场声压级始终大于1阶谷值共振频率激励下获得的驻波场声压级。由此可见,利用扬声器在等截面驻波管中获取大振幅驻波场,驻波管由1阶峰值共振频率激励较为合适。 相似文献
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由直径不同的两级直圆管连接而成的两级突变截面驻波管具有失谐性,即高阶共振频率不是一阶共振频率的整数倍. 两级突变截面驻波管的失谐性质能够很好地抑制一阶共振频率激励下的大振幅非线性驻波畸变产生的高次谐波,从而获得大振幅纯净驻波场. 通过对两级突变截面驻波管失谐性质的研究,采用大功率扬声器正接等措施,利用两级突变截面驻波管的失谐性质在一阶共振频率激励下获得了184 dB的极高纯净驻波场,并对二至五阶共振频率激励下的声场进行了相应的实验研究. 在二阶、四阶共振频率激励下分别获得了180和166 dB波形比较规整的大振幅非线性驻波,并在三阶、五阶共振频率激励下观察到了谐波饱和现象和锯齿波.
关键词:
失谐驻波管
大振幅驻波
畸变
饱和 相似文献
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在驻波法测定声速实验中,根据发射器和接收器之间合成声场的位移波动方程和声压波动方程,用matlab程序模拟了声场和声压的振幅和初相位分布,并对模拟结果进行了分析和讨论。 相似文献
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讨论了两列相向而行、振幅随传播距离增加而线性衰减的相干波叠加后的数学形式,并用计算机模拟了计算结果,得到稳定的驻波波形. 相似文献
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对闭管中有限振幅气柱振动规律进行了数值研究,结果显示有限振幅驻波场具有强烈的非线性特性,在一定条件下会出现分岔混沌现象.倍周期分岔是有限振幅驻波场达到混饨的途径之一. 相似文献
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在一维有限振幅驻波声场中观察到了分岔现象。除了理论所预期的高次谐波存在外,次谐波、分数谐波亦存在于有限振幅驻波声场中。随基波声压级提高,最终达到混饨状态。 相似文献
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驻波法测量声速实验的讨论 总被引:1,自引:4,他引:1
根据声波在2个换能器之间多次反射和声波在空气中的衰减,研究了驻波法测量声速实验中接收器输出信号随接收器到发送器间距离的变化.理论推导结果表明:声波在一般情况下不是严格的驻波,但是当反射比接近-1时则是双曲函数形式的驻波,这与实验测量结果一致.只有接收器到发送器的距离比较远,反射比接近-1时,才能得到几乎理想的驻波. 相似文献
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Two opposite gravity-capillary waves of equal frequency give rise to the formation of a standing wave on the ocean surface and, thus, in the nonlinear approximation, generate a sound wave of twofold frequency with an amplitude proportional to the squared height of the surface wave [1]. This effect, being caused by the nonlinear interaction of opposite surface waves, can give rise to the radiation of sound waves in both ocean and atmosphere [2]. Opposite waves can appear in the ocean as a result of different ocean-atmosphere interactions and, in particular, as a result of the blocking of capillary waves on the slope of a gravity wave. 相似文献
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Recent studies have shown that there is no loss of cell viability when the cells are subjected to ultrasonic standing wave fields in acoustic cell retention systems. These systems are characterised by waves that spatially vary in pressure amplitude in the direction of sound propagation. In this work an anechoic 'one-dimensional' sonication chamber has been developed that produces propagating waves, which differ from standing waves in that the pressure amplitude remains constant as the wave travels in a medium with negligible attenuation. The viability of yeast cell suspensions as a function of treatment time was investigated during exposure to both standing and propagating wave fields with frequencies slightly above 2 MHz. The influence of 12% (vol/vol) of ethanol in water on the spatial arrangement of the cells in suspension was also studied. Changes in yeast cell morphology caused by the different types of suspension media and the ultrasonic treatment were examined by transmission electron microscopy (TEM). The agglomeration of yeast cells within the pressure nodal planes appears to minimise damaging effects due to ultrasonic fields. 相似文献
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驻波声场中悬浮临界密度及稳定性研究 总被引:1,自引:0,他引:1
本文以声场中物体为研究对象,理论上得到行波和驻波场中的声辐射压力方程.在驻波声场中引入临界悬浮密度概念,可作为物体能否在非线性声场中悬浮的判据,同时给出谐振腔移动速度的最大范围.更进一步,以实验参数作为数值计算的输入来指导实验,并结合实验结果讨论了驻波声场中样品密度和大小、发射面和反射面形状以及两者之间的距离、反射面的尺寸等因素对物体悬浮稳定性的影响,发现当物体尺寸和密度确定时,调控好谐振腔的长度,增加波腹处的声压是提升声悬浮稳定性的有效手段. 相似文献
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The standing wave in the near field of the screech jet exhausted from a nozzle with a hard plate works on the jet flow as the forcing wave by the location of a reflecting plate, and then jet flow is considered to be changed. Moreover, the reflector location from the nozzle changes the sound pressure contours of the near field. Intensity maps of the screech tone which indicate the propagation to the jet axial direction or the radial direction of the jet by the presence of the reflector plate have not been explored. In the present paper, acoustic characteristics in the near field of the screech tone with the reflecting plate are studied using an optical wave microphone, which can measure the sound propagating for both vertical and horizontal directions to the jet axis. As a result, the standing wave in the near field of the screech jet with the reflector has two types: One is the standing wave between the hydrodynamic pressure fluctuation propagating jet downstream and the sound pressure propagating upstream, and the other is the standing wave by the difference between the wavelength of the sound wave and the wavelength at the place close to the jet. 相似文献
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V. T. Faerman 《Acoustical Physics》2016,62(1):22-26
Experimental measurements are presented for sound wave attenuation in foam without additives (standing wave method) and in foam with added particles (pulse method). A setup is developed that makes it possible to obtain a standing sound wave in stable foam and estimate the attenuation coefficient. A comparison is made of the coefficients of sound attenuation in foam in the sonic and ultrasonic frequency ranges, which have been published in a number of works. It is shown that the introduction of particles into foam leads to an increase in sound wave attenuation and may be the result of the viscous mechanism of sound wave energy loss. 相似文献
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通过由一个声压换能器和一个质点速度换能器所构成的传感器(p-u声强探头)同时测量材料表面附近的声压和质点振动速度,可直接得到其声学阻抗,进而得到材料的反射因子、吸声系数。本文利用一个p-u探头声强测量系统,在半消声室内测量了三聚氰胺泡沫的吸声系数,分析了声源高度和入射角度、材料样本尺寸和厚度对吸声系数测量的影响,并和阻抗管中测量得到的法向吸声系数进行了对比。最后分析了声阻抗率的幅值和相位误差对吸声系数的影响,推导了它们的误差传递公式。 相似文献
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基于囚禁离子与驻波激光场相互作用,应用驻波光场的相位调制的方法,我们提出了一种制备离子振动压缩态的新方法.研究了压缩振幅与调制振幅的关系.我们发现:适当选择调制振幅,可把离子制备在最佳压缩振动态上,并且它们的产生伴随着自发辐射的相消.提出了一种实验构想,并进行了讨论. 相似文献