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1.
人耳可以分成三部分:外耳、中耳和内耳。外耳包含耳壳、耳道和鼓膜。中耳是一个小腔,有欧氏管通到鼻腔,使鼓膜两侧保持平衡。中耳内有三块听小骨:椎骨、砧骨和镫骨。椎骨连到鼓膜上,镫骨则连到内耳的卵圆窗。三块听小骨的作用是把鼓膜上微弱的振动放大后传入内耳。内耳的听觉部分是耳蜗,它的形状象螺旋管,中间有基底膜把它分隔为两半,膜端有小孔通道。耳蜗内充满淋巴液。基底膜上有柯蒂氏器官,其上有大量灵敏的毛细胞。毛细胞分两层,均匀地分布在基底膜上。外毛细胞把基底膜振动放大并传给内毛细胞,后者的神 相似文献
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针对合金熔体等液体材料的超声处理过程,选取水作为透明模型材料,采用数值模拟计算和示踪粒子实验方法,研究了20和490 kHz两种频率超声作用下水中的声场和流场分布.结果表明,增大变幅杆半径能够提高水中声压水平,扩大空化效应的发生区域.当超声频率为20 kHz时,水中声压最大值出现在超声变幅杆下端面处,且声压沿传播距离的增大而显著减小.如果超声频率增加至490 kHz,水中的声压级相比于20 kHz时明显提高,且声压沿着超声传播方向呈现出周期性振荡特征.两种频率超声作用下水中的流场呈现相似的分布特征,且平均流速均随着变幅杆半径增大表现出先升高后降低的趋势.变幅杆半径相同时,20 kHz频率超声作用下水中的平均流速高于490 kHz频率超声.采用示踪粒子图像测速技术实时观察和测定了水中的流速分布,发现其与计算结果基本一致. 相似文献
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城市噪声作为一种污染源,给人们的生活带来不便;同时噪声中蕴含的能量没有被合理利用,造成浪费。为了解决此问题,该文设计引入了点缺陷的声子晶体、纤维层、压电材料复合结构,对入射噪声进行有效吸收并在点缺陷处对入射声压有较明显的声压加强。采用有限元和边界元的方法,对该复合结构的降噪发电效果进行数值模拟。结果显示在输入声压为2 Pa时,声子晶体结构带隙1.1 kHz处,吸声系数达到0.6,压电片有最高的输出电压0.5 V,输出功率密度达到308.49μW/cm~3。与传统降噪结构相比能更好地实现对声能的吸收与利用。 相似文献
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针对平面型光纤Bragg光栅(Fiber Bragg Grating,缩写为FBG)水听器探头加速度响应明显,影响它对正常声压进行探测的需求,提出了采用加速度补偿措施进行加速度去敏这一有效方法。从理论和实验上分析研究了带加速度补偿平面型光纤FBG水听器探头的结构灵敏度、灵敏度频率响应特性和加速度响应特性。结果表明:采用加速度补偿措施后,单位加速度(1m·s-2)响应输出的等效作用声压由2.52~3.26 Pa降为0.0758~0.217 Pa。同时,探头结构灵敏度由28 fm/Pa减小为20 fm/Pa,动态谐振频率由6.2 kHz增高为6.52 kHz。谐振频率的增加有助于提高水听器系统的动态响应特性,而结构灵敏度的降低,可以通过提高FBG动态波长解调仪的灵敏度来进行补偿。本来,光纤光栅或光纤光栅激光水听器系统可探测灵敏度主要由解调仪灵敏度决定,而不是由探头结构灵敏度决定。所以,该加速度补偿措施具有很大的实用性。 相似文献
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设计了一种原波频率500 kHz、差频范围1~30 kHz的截断宽带参量阵,作为水声材料测量系统的声源。通过分析典型频率下的宽带参量源指向性理论计算和实际测量结果,发现两者结果的曲线基本吻合,证明计算模型是正确的。应用钟形短时脉冲实现水声材料声特性的宽带测量,有益于降低样品边缘衍射干扰。并建立了测量水声材料大面积板状样品声压反射系数、声压透射系数和吸声系数的压力罐测量系统,罐体内尺寸Φ4 m×12 m,最高静水压4.5 MPa,测量频率范围1~30 kHz。对标准样品(尺寸1m×1m)进行了测量实验,其测量结果和理论曲线有很好的吻合,参量源测量法得到了验证;之后,通过对一块橡胶板样品在不同静压力下的吸声性能进行了测量和有效评估,进一步确认了参量源测量法在压力罐这样有限水域中的潜在应用价值。 相似文献
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超顺磁性氧化铁纳米粒子与造影剂微泡结合形成磁性微泡,用于产生多模态造影剂,以增强医学超声和磁共振成像.将装载有纳米磁性颗粒的微泡包膜层看作由磁流体膜与磷脂膜组合而成的双层膜结构,同时考虑磁性纳米颗粒体积分数a对膜密度及黏度的影响,从气泡动力学基本理论出发,构建多层膜结构磁性微泡非线性动力学方程.数值分析了驱动声压和频率等声场参数、颗粒体积分数、膜层厚度以及表面张力等膜壳参数对微泡声动力学行为的影响.结果表明,当磁性颗粒体积分数较小且a≤0.1时,磁性微泡声响应特性与普通包膜微泡相似,微泡的声频响应与其初始尺寸和驱动压有关;当驱动声场频率f为磁性微泡共振频率f0的2倍(f=2f0)时,微泡振动失稳临界声压最低;磁性颗粒的存在抑制了泡的膨胀和收缩但抑制效果非常有限;磁性微泡外膜层材料的表面张力参数K及膜层厚度d也会影响微泡的振动,当表面张力参数及膜厚取值分别为0.2—0.4 N/m及50—150 nm时,可观察到气泡存在不稳定振动响应区. 相似文献
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基于多层膜准单色覆盖50~1500 eV能谱的多能点发射光谱测量系统可获得聚龙一号装置Z-pinch等离子体X射线源的能谱结构和总能量等信息。考虑装置的条件,在13 nm处的多层膜需要工作在掠入射角60。常规的Mo/Si多层膜尽管反射率最高,但其带宽较大,不能满足多层膜准单色的要求。因此提出将Mo和C共同作为多层膜的吸收层材料与Si组成Si/Mo/C多层膜,可使反射率降低较小而带宽明显减小。采用磁控溅射方法制备了Si/Mo/C多层膜,其掠入射X射线反射测量表面多层膜的结构清晰完整,同步辐射工作条件下反射率测量,得到Si/Mo/C多层膜在13 nm处和掠入射角60时的反射率为56.5%,带宽为0.49 nm(3.7 eV)。 相似文献
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黑蚱蝉(Cryptotymrana atrata Fabricius)发声装置的结构和功能 总被引:2,自引:0,他引:2
黑蚱蝉的发声器官是一种小型化的多重组合式发声装置。其鸣声由重复频率约180Hz的调幅脉冲列组成,可见带宽200—12500Hz,主峰频率5kHz。鼓膜的振动发声是由两侧鼓膜肌交替收缩驱动的。鼓室的功能是改善波形、调谐特性和扩声。腹室的功能是进一步改善音色和扩声。腹腔的主要功能是提高输出功率。褶膜对改善音色和调谐特性有明显的作用。腹瓣和镜膜仅对音量调节有一定的影响。 这些结果可为声学装置的研究提供一种生物原型。 相似文献
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运用光谱技术研究了椎骨组织不同位置的特征识别因子.光谱采集系统由双光纤手钻一体式探头(光纤芯径200 μm,中心距离0.5 mm)、卤素光源(波长360~2 000 nm)、光纤光谱仪(检测波长为200~1 100 nm)和计算机组成,可以同时获得生物组织的漫反射光谱和约化散射系数.以猪椎骨为实验对象,测量椎弓根螺钉植入针道上不同骨组织的漫反射光谱和约化散射系数,并对光谱进行特定波长的峰值、面积、斜率分析,获得特性识别因子.研究发现,椎弓根钉植入针道上不同骨组织的光谱表现出不同的变化特性.其中峰值的变化比约化散射系数的变化高1.88倍,面积的变化比约化散射系数的变化高2.05倍.在495~505 nm处,骨密质和骨疏质的光谱斜率都为正值;在520~535 nm处,骨密质光谱的斜率为正值,而骨疏质光谱的斜率为负值.结果表明,通过光谱特性分析获得的峰值、面积和斜率因子能够有效地区分针道上骨密质与骨疏质的差异. 相似文献
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Coupling of somatic electromechanical force from the outer hair cells (OHCs) into the organ of Corti is investigated by measuring transverse vibration patterns of the organ of Cori and tectorial membrane (TM) in response to intracochlear electrical stimulation. Measurement places at the organ of Corti extend from the inner sulcus cells to Hensen's cells and at the lower (and upper) surface of the TM from the inner sulcus to the OHC region. These locations are in the neighborhood of where electromechanical force is coupled into (1) the mechanoelectrical transducers of the stereocilia and (2) fluids of the organ of Corti. Experiments are conducted in the first, second, and third cochlear turns of an in vitro preparation of the adult guinea pig cochlea. Vibration measurements are made at functionally relevant stimulus frequencies (0.48-68 kHz) and response amplitudes (<15 nm). The experiments provide phase relations between the different structures, which, dependent on frequency range and longitudinal cochlear position, include in-phase transverse motions of the TM, counterphasic transverse motions between the inner hair cell and OHCs, as well as traveling-wave motion of Hensen's cells in the radial direction. Mechanics of sound processing in the cochlea are discussed based on these phase relationships. 相似文献
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Asynchronous neural activity recorded from the round window 总被引:1,自引:0,他引:1
D F Dolan A L Nuttall G Avinash 《The Journal of the Acoustical Society of America》1990,87(6):2621-2627
Voltage recorded from an electrode on the round window (RW) of guinea pig has characteristics that reflect the activity of auditory-nerve fibers in the absence of acoustic stimulation. Fast Fourier transformation (FFT) of the noise recorded from the RW electrode shows a broad spectral peak from 0.8-1.0 kHz. The magnitude of the biological noise is increased by high-frequency, bandlimited acoustic noise stimulation. Pure tones can suppress or enhance the spectral components around 0.8-1.0 kHz depending on frequency and intensity. Kainic acid applied to the intact RW membrane eliminates the biological noise (and the evoked cochlear whole-nerve responses) without alteration of the cochlear microphonic or the summating potential. The spectral characteristics of the biological noise seem to be related to the elemental waveform contributed by the individual auditory-nerve fibers to the voltage recorded at the RW electrode [Kiang et al., Electrocochleography, edited by R. J. Ruben, C. Elbering, and G. Solomon (University Park, Baltimore, 1976)]. 相似文献
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For 68 temporal bones, frequency curves for the round window volume displacement have been measured for a constant sound pressure at the eardrum. Phase curves were measured for 33 of the specimens. The levels averaged amplitude curve is approximately flat below 1 kHz, where the round window volume displacement per unit sound pressure at the eardrum is 6.8 X 10(-5) mm3/Pa, and falls off by about 15 dB/oct at higher frequencies. For the 20 ears having the largest sound transmission magnitude at low frequencies, the corresponding amplitude curve is displaced about 5 dB towards higher levels. The phase of the round window volume displacement lags the eardrum sound pressure phase. In average for 33 temporal bones, the phase lag increases from zero at the lowest frequencies to pi near 2 kHz and to about 1.5 pi at 10 kHz. 相似文献
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Brass D 《The Journal of the Acoustical Society of America》2000,107(2):894-907
The post-mortem transfer function of the cochlea of the guinea pig was compared to the transfer function generated by a model with parameters derived from physical measurements of the guinea pig cochlea. Both the formulation and parameters of the model were carefully chosen to be realistic using evidence from published measurements. The fit between the transfer function of the model and recent mechanical measurements of the passive guinea pig cochlear response was good, with a root mean square ratio of 6.3 dB in amplitude and 0.33 pi rad in phase. The model was used to explore the effect of cochlear partition mode factor and duct geometry upon the mechanical response of the cochlea. Possible inadequacies of the model which could explain the remaining differences between the output of the model and measurements are discussed. 相似文献
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Marquardt T Hensel J Mrowinski D Scholz G 《The Journal of the Acoustical Society of America》2007,121(6):3628-3638
Previous physiological studies investigating the transfer of low-frequency sound into the cochlea have been invasive. Predictions about the human cochlea are based on anatomical similarities with animal cochleae but no direct comparison has been possible. This paper presents a noninvasive method of observing low frequency cochlear vibration using distortion product otoacoustic emissions (DPOAE) modulated by low-frequency tones. For various frequencies (15-480 Hz), the level was adjusted to maintain an equal DPOAE-modulation depth, interpreted as a constant basilar membrane displacement amplitude. The resulting modulator level curves from four human ears match equal-loudness contours (ISO226:2003) except for an irregularity consisting of a notch and a peak at 45 Hz and 60 Hz, respectively, suggesting a cochlear resonance. This resonator interacts with the middle ear stiffness. The irregularity separates two regions of the middle ear transfer function in humans: A slope of 12 dB/octave below the irregularity suggests mass-controlled impedance resulting from perilymph movement through the helicotrema; a 6-dB/octave slope above the irregularity suggests resistive cochlear impedance and the existence of a traveling wave. The results from four guinea pig ears showed a 6-dB/octave slope on either side of an irregularity around 120 Hz, and agree with published data. 相似文献
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W S Rhode 《The Journal of the Acoustical Society of America》1978,64(1):158-176
A set of experiments was conducted using the M?ssbauer effect to determine the vibratory characteristics of the basilar membrane, Reissner's membrane, the malleus, incus, and oval window in squirrel monkey. A few measurements were also made in guinea pig in the basal cochlear region. The nonlinear vibration properties of the basilar membrane are described in detail for the midfrequency region in the squirrel monkey. Only in this region have nonlinear effects been observed. A comparison of mechanical and neural data indicates good qualitative agreement. 相似文献
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Two-dimensional analysis of fluid motion in the cochlea resulting from compressional bone conduction
Fluid motion resulting from the compressional excitation of the cochlear capsule due to bone conduction is examined in this paper. Vibrations of the skull deform the shape of the cochlear capsule and give rise to motion the fluid. A two-dimensional channel having a height to length ratio equal to ε is used to model the cochlea. The cochlear pressure is expressed as an integral equation in the cochlear partition velocity. In the limit as ε approaches zero the integral equation is solved and the cochlear pressure is expressed as an asymptotic expansion in ε. Rapid spatial variation in the velocity of the cochlear partition requires one to treat high-order fluid modes within the cochlear fluid. Hence, evanescent pressure modes are included in the analysis. Asymmetry in the oval and the round window velocity is shown to give rise to a pressure gradient across the cochlear partition and basilar membrane displacement. The vibration amplitude of the cochlear partition is shown to depend on the value of the ratio of the oval and the round window impedance. 相似文献
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Basilar membrane mechanics at the base of the chinchilla cochlea. I. Input-output functions, tuning curves, and response phases 总被引:2,自引:0,他引:2
L Robles M A Ruggero N C Rich 《The Journal of the Acoustical Society of America》1986,80(5):1364-1374
Basilar membrane (BM) velocity was measured at a site 3.5 mm from the basal end of the chinchilla cochlea using the M?ssbauer technique. The threshold of the compound action potential recorded at the round window in response to tone bursts was used as an indicator of the physiological state of the cochlea. The BM input-output functions display a compressive nonlinearity for frequencies around the characteristic frequency (CF, 8 to 8.75 kHz), but are linear for frequencies below 7 and above 10.5 kHz. In preparations with little surgical damage, isovelocity tuning curves at 0.1 mm/s are sharply tuned, have Q10's of about 6, minima as low as 13 dB SPL, tip-to-tail ratios (at 1 kHz) of 56 to 76 dB, and high-frequency slopes of about 300 dB/oct. These mechanical responses are as sharply tuned as frequency-threshold curves of chinchilla auditory nerve fibers with corresponding CF. There is a progressive loss of sensitivity of the mechanical response with time for the frequencies around CF, but not for frequencies on the tail of the tuning curve. In some experiments the nonlinearity was maintained for several hours, in spite of a considerable loss of sensitivity of the BM response. High-frequency plateaus were observed in both isovelocity tuning curves and phase-frequency curves. 相似文献