| 1. | Finally, we determine the changes in the phases of the components of the reflected and the incident wave .
最后，我们求反射波和入射波各分量的位相变化。 |
| 2. | By reducing the feedback of the cavity, a laser will no longer be self oscillatory but it will amplify an incident wave which has triggered stimulated emission .
减小腔的反馈，激光器就不再会自己振荡，而只是放大触发受激发射的入射波。 |
| 3. | Alternatively, we can image that the incoming wave is diffracted by the object and the resulting diffracted wave is then diffracted again by the objective lens .
换一种方式，我们可以这样想象：入射波被物体反射，所得到的衍射波再一次受到物镜的衍射。 |
| 4. | During the processing , there is only a start point of input strain that needs to find
在程序中，根据波形的特点初步确定入射波的起点。 |
| 5. | When an incident optical beam is bright solition , this beam propayates along a linear path with its shape kept unchanged
入射波为明孤子波时，能够在对数型非线性电介质中稳定传播。 |
| 6. | At the end of this chapter , a new inciding wave source using in simulation regular waveguides by fdtd method is given ,
最后本文还用离散傅立叶变换方法给出了用于fdtd方法研究规则波导问题中的入射波源。 |
| 7. | The reason for the emergence of this phenomenon is that the frequency of incident microwave is getting close to the eigenfrequency of the cavity
这是因为此时腔体的本征频率,近似等于入射波载频,引起腔体的共振。 |
| 8. | Computation of first - order wave force was simplified , and second - order wave force included second diffraction of second - order incident wave
对一阶波浪力计算进行了进一步的简化，在二阶力的波浪力计算中考虑了二阶入射波的二次绕射。 |
| 9. | As an example , the oscillation of a rectangular harbour due to the incident waves with different directions and wave numbers was investigated
作为算例，就一矩形港湾在不同方向、不同波数入射波情况下的港内水波振动问题进行了计算分析。 |
| 10. | The influences of wave numbers , angle of incidence , combination of different media parameters and cavity shape upon the dscf around the cavity are discussed
讨论了入射波数、入射角、不同介质组合以及孔的形状对孔附近动应力集中系数的影响。 |
