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扰动波的英文

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"扰动波"怎么读用"扰动波"造句

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  • perturbation wave
  • wavelet

例句与用法

  • Furthermore , with the fourier series technique , the disturbance is discomposed into predominant mode and high frequency harmonics , and the nonlinear stability of the nonparallel boundary layer is studied
    采用fourier级数的方法把扰动波分解为基本模态和高频谐波模态,导出非平行非线性抛物化稳定性方程。
  • With the fourier series technique , the disturbance is discomposed into predominant mode and high frequency harmonics . the nonlinear stability of three - dimensional disturbances for the blasius boundary layers is studied
    借助fourier级数的方法将扰动波分解为基本模态和高频模态,研究了三维扰动的非线性边界层稳定性问题。
  • Using the two - stream fluid model , the linear dispersion relation is derived assuming a two - dimensional spatial geometry . two cases are considered , one is that the 2d spatial geometry is defined by the plane containing the two counterstreaming electron populations and the perturbation wave vector ( referred as the xy plane ) , and the other is that the geometry is defined by the plane being vertical to the two counterstreaming electron populations ( referred as the yz plane )
    对高能束流和电子回流构成的双流系统,建立冷等离子体流体模型,采用简正模分析方法,分别考虑扰动波矢在平行于电流传播方向的平面(记为xy平面)上和在垂直于电流传播方向的平面(记为yz平面)上这两种情况,推导了不稳定性的色散关系。
  • Generally , tidal bore is wave alignment moving upstream estuary , and its surface will break when the wave alignment is strong , which leads to water roll tracing the source . the velocity , which is between small - disturbed wave velocities before tidal bore happens and the one after tidal bore happens , increases with the ratio of tidal bore height to the water depth in wave front
    涌潮一般是向河口上游推进的波列,强度大时,表面破碎,进而发展成溯源推进的水滚,其传播速度随涌潮高度与波前水深比值增加,大小介于涌潮前后小扰动波波速之间。
  • The shearing layer is carried by the jet and the eddy is formed because of the instability and selective amplification of shearing layer which will propagate to the downstream . as the eddy impacts the impinging wall , a wave of pressure disturbance with certain frequency is induced . this wave then propagates to the upstream with high speed , and results in the overlap and amplification of the waves when the frequencies of them are close with each other
    当前喷嘴流束中的不稳定扰动波在穿过腔内的剪切层时,剪切层对其有选择放大作用,形成涡环结构,剪切流动中涡环与碰撞壁撞击,在碰撞区域产生压力扰动波并向上游反射,在上游剪切层分离处诱发新的扰动的产生,当新扰动与原扰动匹配时,射流上游就被不断地受到周期性激励,腔内就产生流体自激振荡并在后喷嘴出口形成脉冲射流。
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