Relativistic Doppler Shift相对论多普勒效应 The normal Doppler shift for waves such as sound which move with velocities v much less than c is given by the expression 对于速度v远小于c的波,如声波,其多普勒频移由下式给出
![]() where the plus sign is taken for waves traveling away from the observer. For light and other electromagnetic waves, the relationship must be modified to be consistent with the Lorentz transformation and the expression becomes 其中,正号表示波是远离观察者传播的。对于光和其他电磁波,关系式必须修改以与洛伦兹变换一致,表达式则变为
![]() Here v is the relative velocity of source and observer and v is considered positive when the source is approaching. 这里v是声源和观察者的相对速度,当声源靠近时,v被考虑为正数。
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Doppler Effect, Electromagnetic Waves多普勒效应,电磁波
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Fractional Wavelength Change波长分数变化 For purposes of determining recession speed of stars and galaxies with the Doppler effect by observation of the red shift of spectral lines, it is convenient to express the Doppler effect in terms of the shift in wavelength compared to the source wavelength. For these purposes it is more convenient to define a receding velocity as positive in the wavelength relationship: 为了通过观测谱线的红移来确定恒星和星系的退行速度,使用多普勒效应时,将波长与源波长的差异来表达多普勒效应是方便的。对于这些目的,更方便的是将退行速度定义为波长关系中的正数:
![]() The fractional wavelength change is defined as the z parameter for characterizing red shifts: 波长的分数变化定义为z参数,用于表征红移:
![]() In terms of the usual relativity symbols, this becomes 在通常的相对论符号中,这变为
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Doppler Frequency多普勒频率
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