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The relationship between acoustic wave direction,laser incident angle,and laser diffraction angle of TeO2 acousto-optical deflector with acoustic frequency was analyzed based on the TeO2 crystal acousto-optical characteristic and Dixon equations under abnormal Bragg diffraction.

根据晶体的声光特性以及反常布喇格衍射的Dixon方程,得出了氧化碲声光偏转器在反常布拉格衍射条件下的参量矢量关系。分析了超声波方向、入射光角度、衍射光角度与声波频率之间的关系。

The results are in good agreement with the experimental results.(2) According to the obtained relation between electromagnetic wave and incident stress wave and the resolution of the transmitted coefficients in the joint,the strength variation of the EME before and after the joint when the normal incident stress wave propagates to the linear deformative joint has been presented.

2依据所得到的电磁波与入射应力波之间的关系及应力波在节理面处的透射解,获得垂直入射应力波作用下产生的电磁波在线性变形节理面前后的强度关系。

It can be concluded that, when the jet is injected at positive angles, the initial section of the jet increases and the region affected by the jet decreases in the vertical direction; moreover, the circumfluence toward the jet exit becomes more obvious, and the separation events in the lee of the jet weaken. When the jet is injected at negative injection angles, it disarranges the flow upstream and the curvature of jet trajectories varies smartly along the flow direction.

结果表明:射流正向倾斜入射时,射流起始段增加,在垂直方向对主流场的影响区域减小,射流喷口上游位置处的&孔吸流动&更为明显,射流出口下游背风侧的分离现象逐渐减弱;射流反向倾斜入射,对上游流场的扰动增加,射流在弯曲段内曲率变化大。

First, the background spectrum is subtracted from experimental one; Second, by the spectrum stripping, the counts came from partial energy deposition of incidence photon in HPGe crystal, such as Compton scatting or pair production; the next, transform the experimental spectrum to the incidence photon flux spectrum.

实验数据的处理过程有三步:1 从实验谱中减掉本底谱;2 实验谱中分离掉各种能量的入射光子在晶体中的部分能量沉积(康普顿散射、电子对效应):3 处理过的实验谱转成入射光子通量谱。比较结果显示,在本实验中,模拟谱对实验谱的总计数相对偏差不大于20%,两者基本符合。

Simulation results show that both the longitudinal and transverse wave are included in the reflected waves,the reflection coefficient of longitudinal wave augments with the increase of the incident angle,and the reflection coefficient of transverse wave augments first and then minishes,the transverse wave disappears when the incident angl.

主要研究了声波从粘弹性介质向流体介质斜入射情况下的声反射特性,分析表明:反射声波中有横波和纵波同时存在,纵波声压反射系数随入射角度的增大逐渐增大,横波的声压反射系数随入射角度的增加先增大后减小,在垂直入射时只有纵波,而没有横波存在。

The algorithm only needs to solve an ill-posed linear system and a well-posed minimization problem and requires only the knowledge of the near field measurements of the scattered fields due to point source fields at a finite number of incidence and observation points distributed over a limited aperture.

该算法只需求解一个不适定的线性系和一个适定的非线性最小化问题,而且只需要点源入射场的散射场在某个有限孔径中若干有限个入射和测量点上的近场测量信息。

The transit time and gain curves are obtained in the simulation.

获得了光电子的倍增次数随入射时刻而变化,并在考虑了入射电子为一高斯电子脉冲的情况下,分析了选通脉冲的幅度、宽度和波形对选通特性的影响。

The accuracy of present numerical model is verified by the simulation of a rectangular harbor with constant water depth. For Taipei Harbor calculations, three incident wave directions, namely, WNW, N and NNE, together with constant water depth of 10m are considered.

接著考虑台北港第三期配置,使用三个波波浪入射方向与代表性水深(10m),配合港区码头位置的选定,计算入射波浪周期与波高放大因子的关系,同时由共振周期计算港域波浪场的分布情形,藉以了解台北港第三期规划案港池振荡的特性。

When 1053 nm 20 ns Nd:YLF laser was used as pump in a 3∶1 inverse expansion system are using attenuators to adjust input energy in the rang of 2 to 92 mJ, the rules of transmitted energy and waveform versus input energy are acquired, and compared with the results of focusing pump.

以波长1053nm、脉宽20 ns的Nd:YLF激光器为光源,采用3∶1的缩束系统,通过衰减片调整入射光能量在2mJ—92mJ变化,获得了透射光能量和功率波形随入射能量变化的规律,并与聚焦条件下的结果进行了比较。

The number of iterations and multiplications required by this method is approximately 10% that required by the available methods when only one path is received and this will be further reduced to 2% that when two paths exist.

单信号入射时本方法的迭代次数和乘法次数约为同类方法的10%,双信号入射时的计算量进一步减小至同类方法的2%。

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In the negative and interrogative forms, of course, this is identical to the non-emphatic forms.

。但是,在否定句或疑问句里,这种带有"do"的方法表达的效果却没有什么强调的意思。

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