共查询到19条相似文献,搜索用时 109 毫秒
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为了使共振音叉达到较好的效果,自制了一对共振音叉的悬挂装置及其附件,用该装置可以将2个共振音叉悬挂起来,其演示效果较好.同时,本文探讨了共振音叉不同的悬挂方式,并介绍了如何演示共鸣实验和利用该装置演示声波的干涉实验. 相似文献
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利用自制的拾音器,把音叉共鸣微弱的机械振动转换成电信号,送入护音器放大,得到宏量的音叉共鸣声,显著提高了音叉共鸣演示实验的效果。 相似文献
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用音叉演示声音共鸣的过程是:取两个频率相同的音叉A和B,将它们插在共呜箱上摆放在一起.用橡皮糙敲击音叉A的叉股,使音叉A发声.过一会儿,用手按住音叉A的叉股,使它停止振动,这时音叉A不发声了,却听到音叉B在发声.实际作这个实验时,因音叉选取不当,或操作方法不妥,音叉B发出的声音因响度不够,实验效果很不明显,根据经验,共鸣实验演示成功的关键,应注意以下几点.1.音叉和共鸣箱选取要合理.发生共鸣时,原先不发声的音叉必须从声波中获得足够大的能量,才有较大的响度,共呜声才明显,因此实验时应选用发声功率较大的… 相似文献
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通常演示声音的共鸣时是把两个音叉分别插在两个共鸣箱上,开口相对放在相距50厘米左右的地方,激发其中的一个,过2—3秒钟后,用手按抚使其不响,但能听到另一个音叉的声音。这种演示方法,另一个音叉的声音很微弱,特 相似文献
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振动合成演示实验,通常要用到共鸣音叉,电子示波器等设备.共鸣音叉的振动是阻尼振动,能量小,衰减快,振幅不易控制.当观察者距离较远时,就很难听到音叉振动的声音,更看不到音叉振动.用电子示波器可以显示振动图象、振动合成图形;但对初学者来说,如能看到振动合成的过程,将更有助于对“合成”的理解.这里介绍一个简单的方法,用激光将机械振动放大投影到屏幕上,使观察者不仅闻其声,观其形,还可看到振动合成的全部过程。此外,在传统的实验中运用激光技术,也会给人留下深刻的印象.实验原理及装置 将平行光束入射到振动平面上,再反射到屏幕.(见图1… 相似文献
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在波动演示实验中引入驻波的尝试朱连喜.(江苏省药科学校镇江212003)用驻波(电动音叉)演示波的干涉,可弥补水波干涉的不足,能收到较好的效果.1驻波演示实验如图1所示,P是电动音叉,弦线一端A系在音叉上,另一端通过滑轮系一砝码,以使弦线拉紧,使电动... 相似文献
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驻波演示实验常用音叉作振源.音叉末端系一软线,在线上形成驻波.但因音叉末端振动的振幅较小(约一毫米)。驻波波腹处的振幅也不大(约几毫米),所以在教室中演示不醒目.笔者用微型直流电机(玩具汽车上小电动机)代替音叉,线上驻波波腹处的振幅可达数厘米,在教室中演示很明显,学生便于观察,效果不差.实验设备也简单轻巧,携带方便. 如图所示.电动机需1.5伏直流电源(一节一号电池即可),电流约0.2安培,转速约每秒数十转.小轮可用0.5 × 15厘米胶布盘绕在电动机的转轴上即成.用一小铁钉插入小轮中成为偏心轴,其上套一可活动的金属套管.棉线系在套管… 相似文献
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为了进一步提高基于泛频振动的石英增强光声光谱测声器探测灵敏度,在一次泛频振动模式下采用一个比商用标准音叉外形尺寸大5倍的定制大音叉,并对其性能进行优化.通过理论和实验研究得出了音叉与激光的最佳作用位置,发现音叉的一次泛频振动有两个波腹点,且在距离音叉根部8 mm处,音叉振臂的振动幅度最大.微型声音谐振腔由三种不同内径的不锈钢毛细管加工而成,与音叉组成共轴配置石英增强光声光谱光谱测声器,用来进一步增强信号幅值.在最佳微型声音谐振腔配置下,获得了30倍的信号增益因子,有效提高了石英增强光声光谱光谱测声器的探测灵敏度. 相似文献
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文中对自制对称正型音叉与自制非对称异型音叉受力F后音叉产生的振动的现象进行了研究,用DIS声传感数字化信息系统采集振动频率,研究频率与音叉叉股长度的关系,从而对音叉叉股对称与非对称的情况进行研究。 相似文献
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N. Petra J. Zweck A. A. Kosterev S. E. Minkoff D. Thomazy 《Applied physics. B, Lasers and optics》2009,94(4):673-680
Quartz-enhanced photoacoustic spectroscopy (QEPAS) sensors are based on a recent approach to photoacoustic detection which
employs a quartz tuning fork as an acoustic transducer. These sensors enable detection of trace gases for air quality monitoring,
industrial process control, and medical diagnostics. To detect a trace gas, modulated laser radiation is directed between
the tines of a tuning fork. The optical energy absorbed by the gas results in a periodic thermal expansion which gives rise
to a weak acoustic pressure wave. This pressure wave excites a resonant vibration of the tuning fork thereby generating an
electrical signal via the piezoelectric effect. This paper describes a theoretical model of a QEPAS sensor. By deriving analytical
solutions for the partial differential equations in the model, we obtain a formula for the piezoelectric current in terms
of the optical, mechanical, and electrical parameters of the system. We use the model to calculate the optimal position of
the laser beam with respect to the tuning fork and the phase of the piezoelectric current. We also show that a QEPAS transducer
with a particular 32.8 kHz tuning fork is 2–3 times as sensitive as one with a 4.25 kHz tuning fork. These simulation results
closely match experimental data. 相似文献
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石英音叉作为力传感器广泛地应用于各种扫描探针显微镜,主要涉及石英音叉的同相振动和反相振动两种振动模式.通过实验方法和有限元仿真方法对石英音叉的两种振动模式进行研究,发现石英音叉的双臂之间以及双臂与音叉的基部之间都存在耦合作用,双臂之间的耦合使音叉的反相共振频率升高,双臂与基部之间的耦合使音叉的同相共振频率降低.针对两种振动模式的动态特性建立了石英音叉的机械模型并进行合理简化.简化模型是一个四弹簧三质点系统,计算了简化模型的参数.通过一个音叉臂等效质量变化与音叉反相共振频率变化之间的定量关系证明了简化机械模
关键词:
扫描探针显微镜
石英音叉
振动模式
机械模型 相似文献
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Sangmin An Kunyoung Lee Bongsu Kim Jongwoo Kim Soyoung Kwon Qhwan Kim Manhee Lee Wonho Jhe 《Current Applied Physics》2013,13(9):1899-1905
We have introduced a simple but robust approach to realize stray-capacitance compensation of a quartz tuning fork force gradient sensor by using a tied-prong of the same tuning fork instead of using a variable precision capacitor. The results of quantitative force measurements with the proposed device show excellent agreement with the numerical method of cancellation via the theoretical compensation method with the resonance response curves. Futhermore, the mechanical properties of the condensed nano-water bridges are investigated with the proposed compensator, which provides the potential promise of the intrinsic quartz tuning fork for a quantitative precision force spectroscopy. 相似文献
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M.D. Wojcik M.C. Phillips B.D. Cannon M.S. Taubman 《Applied physics. B, Lasers and optics》2006,85(2-3):307-313
We demonstrate the performance of a novel infrared photoacoustic laser absorbance sensor for gas-phase species using an amplitude-modulated quantum cascade (QC) laser and a quartz tuning fork microphone. The photoacoustic signal was generated by focusing 5.3 mW of a Fabry–Pérot QC laser operating at 8.41 μm between the tines of a quartz tuning fork which served as a transducer for the transient acoustic pressure wave. The sensitivity of this sensor was calibrated using the infrared absorber Freon 134a by performing a simultaneous absorption measurement using a 31-cm absorption cell. The power and bandwidth normalized noise equivalent absorption sensitivity (NEAS) of this sensor was determined to be D=2.0×10-8 W cm-1/Hz1/2. A corresponding theoretical analysis of the instrument sensitivity is presented and is capable of quantitatively reproducing the experimental NEAS, indicating that the fundamental sensitivity of this technique is limited by the noise floor of the tuning fork itself. PACS 43.60.Vx; 43.58.Wc; 43.58.Hp; 84.40.Xb 相似文献