【读书2】【2014】基于MATLAB的雷达信号处理基础(第二版)——测量多普勒频移:空间多普勒(1)

2.6.3测量多普勒频移:空间多普勒

2.6.3. Measuring Doppler Shift: Spatial Doppler

在大多数情况下,雷达观测到的多普勒频移太小,无法从单个脉冲回波中测量。

The Doppler shiftsobserved in radar are too small to be measured from a single pulse echo in mostcases.

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即使对于10 kHz的高多普勒频移和30 dB的信噪比(χ = 1000),Tobs也必须大于123 μs。

Even for a ratherhigh Doppler shift of 10 kHz and a very good SNR of 30 dB (χ = 1000), Tobsmust be much larger than 123 μs.

因此,用单脉冲测量多普勒频移要求脉冲长度大于1 ms,远大于通常使用的亚毫秒(通常小于100μs)脉冲长度。

To measure theDoppler shift with a single pulse would therefore require pulse lengths greaterthan 1 ms, much longer than the submillisecond (usually less than 100 μs) pulselengths typically used.

对于1-kHz多普勒频移和20分贝信噪比,则需要一个持续时间超过10毫秒的脉冲。

For a 1-kHz Dopplershift and 20-dB SNR, a pulse longer than 10 ms would be needed.

由于这个原因,大多数雷达不在脉冲内测量多普勒频移,尽管一些专为超高速目标(卫星和导弹)设计的长脉冲可以做到这一点。

For this reason, mostradars do not measure Doppler shift on an intrapulse basis, although a fewdesigned for very high speed targets (satellites and missiles) and using verylong pulses can do so.

利用多脉冲可以获得所需的长观测时间。

The long observationtime needed can be obtained by using multiple pulses.

假设在t = mT时刻发射一系列M个持续时间为τ的脉冲,其中T为脉冲重复间隔(PRI)。

Suppose a series of Mdistinct pulses of duration τ are transmitted beginning at times t = mT, whereT is the pulse repetition interval (PRI).

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——本文译自Mark A. Richards所著的《Fundamentals of Radar Signal Processing(Second edition)》

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转载自blog.csdn.net/weixin_42825609/article/details/88613631