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Based on the above theories, some vibration characteristics of longitudinal acoustic horns are analyzed with finite element analysis software ANSYS. Some factors influence to large end amplitude distribution is studied such as big end diameter, length of horn, and diameter ratio of big end to small one. In addition, we carry on analysis and research to resonance frequency of large cross-section acoustic horn, amplitude magnification factor, wave node position of horn, transverse vibration situation and so on, and some related change rules are obtained.

在此基础上,通过有限元分析软件ANSYS对纵向超声变幅杆进行了振动特性分析,研究了变幅杆的大端直径、变幅杆长度、大小端面直径比对大端面振幅分布的影响,并对大截面变幅杆的谐振频率、振幅放大系数、变幅杆的波节点位置,横向振动分布等进行了分析研究,总结了相关的变化规律。

The shaker mount is first moved a small distance toward the arch ends to ensure that the arch possesses two stable equilibrium positions, one on each side of the base line. The spring connecting the arch end and the mechanical shaker is carefully chosen such that small shaker stroke can induce large vibration amplitude of the arch.

此外,我们在激振器与拱形梁之间外加一个弹簧做连接,这可使激振器在仅能达到有限的激振振幅下,仍能使拱形梁端点有足够大的振幅产生,并使之能够发生折断式挫曲现象。

The points of maximum amplitude are called antinodes.

振幅最大的点称为波腹,振幅为零的点称为波节。

In the thesis, I introduce a new method to calculate the amplitude for gluon radiation on the base of helicity amplitude approximation.

在本文的研究中,我们还介绍了螺旋振幅近似的计算方法,并在此基础上发展了一种计算胶子辐射振幅的新方法。

The general shape of the amplitude of the vibrating string is a shallow curve that begins at one end of the string, is a maximum at the string's mid-span, and ends at the other end of the string, with the amplitude diminishing over time.

在一般的情况下,琴弦振幅的形状是一道很浅的弧线,它从弦的一端开始,到琴的中部是幅度最高,随着时间振幅不断减少,在弦的另一端消失。

Firstly, the mechanism of heat transfer enhancement by oscillation heat surface is discussed in natural convection scene. For different oscillation amplitude and Rayleigh number, the frequency that the heat transfer rate of oscillation heat surface is higher than non-oscillation condition is found and called critical oscillation frequency. The limitation enhancement of similar physical model is still researched by this study in mixed and forced convection scenes for different amplitude and Grashof number. Generally, that a heat surface subject to a oscillation motion is advantageous to convective heat transfer is a well-known tuition.

首先探讨在垂直管道内振动高温面於自然对流领域内提升高温面热传效率的机制,并且针对不同的振幅与雷利数求得加入振动条件后,高温面散热效果可以优於稳态非振动高温面散热效果的临界振动频率;进而探讨当垂直管道流进入混合对流与强制对流范围时,在不同的振幅与葛瑞秀夫数下,亦可发现加入振动条件后,振动高温面之散热效果可以优於稳态非振动高温面散热效果的临界振动频率。

Firstly, the mechanism of heat transfer enhancement by oscillation heat surface is discussed in natural convection scene. For different oscillation amplitude and Rayleigh number, the frequency that the heat transfer rate of oscillation heat surface is higher than non-oscillation condition is found and called critical oscillation frequency. The limitation enhancement of similar physical model is still researched by this study in mixed and forced convection scenes for different amplitude and Grashof number.

首先探讨在垂直管道内振动高温面於自然对流领域内提升高温面热传效率的机制,并且针对不同的振幅与雷利数求得加入振动条件后,高温面散热效果可以优於稳态非振动高温面散热效果的临界振动频率;进而探讨当垂直管道流进入混合对流与强制对流范围时,在不同的振幅与葛瑞秀夫数下,亦可发现加入振动条件后,振动高温面之散热效果可以优於稳态非振动高温面散热效果的临界振动频率。

The results show that the atomic population is time-independent provided that the atoms are in |β11〉 state. For the other three Bell states, there will appear the periodical collapse revival of atomic populationif the initial mean photon number reaches some special values. With the increase of the initial mean photon number, the oscillation frequency of the time-evolution of atomic population increases correspondingly, and the amplitude decreases. The degree of the entanglement of the two-mode entangled coherent field has no

结果表明,当双原子体系的初态为|β11〉时,原子布居均不随时间变化;当双原子体系的初态为|β00〉,|β01〉或|β10〉且初始平均光子数达到一定值时,演化特性呈现周期性的崩塌-回复效应,并随初始光子数的增加,其演化曲线的振荡频率增大,振幅减小;双模纠缠相干光场的纠缠程度不影响Rabi振荡频率,但对振幅影响显著; Kerr介质与光场耦合系数达到一定值时,对Rabi振荡频率和幅度及原子布居的崩塌-回复周期产生强烈影响。

Fractional revivals,however,are not exactlyhierarchical in amplitude;in other words,their amplitudes are not certain to de-crease with the increase of p,unless the signal mode is very strong.

然而,分数恢复的振幅并不是严格分级的。换言之,它们的振幅并不是一定随p的增加而减小,除非信号模很强。

In the protanopes,the shorter latencies of N1 ,P1,N2 and greater amplitudes of N1-P1,P1-N2 appeared in 520~530nm and 570nm,forming the two-thoughs and two-peaks shapes,with the shortest latencies and the greatest amplitudes in 520~530nm.

先天性红色盲则分别在520~530nm和570nm处潜伏期较短而振幅较大,形成双谷样和双峰样改变;最短潜伏期和最大振幅位地520~530nm处。

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