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Aug 10, 2020

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range observations of single scatterer within synthetic aperture

Single scatterer

Symmetric, doppler center freqency = 0

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range observations as function of radar position

Just rearrange the range observations so they are a function of sensor position rather than being radiallyoriented

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range observations appear as quadratic function

Range, modulo 2*pi, = phase

Quadratic phase = linear frequency

( d/dt (phase) = frequency )

Therefore Azimuth response to single scatterer is LFM “chirp” just like range

The two are sometimes called “fast time”(range) and “slow time” (azimuth)

It only works because it is coherent – the clock/oscillator runs continuously

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3COS(Azimuth Phase) = Azimuth Chirp / No Squint, Doppler c.f. = 0

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18range observations of single scatterer within synthetic aperture

Single scatterer

Not symmetric about the broadside position, therefore dopplercenter frequency will be nonzero. Plus or minus depending on whether skewed to left or right. You must estimate this to construct azimuth reference function.

It means the antenna is pointed a little forward or backward (squinted) from 90 deg to motion vector. In theory can control by “yaw steering”

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18range observations as function of radar position

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18range observations appear as quadratic function

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3COS(Azimuth Phase) = Azimuth Chirp / Squinted, Doppler c.f. != 0

Page 21: 1 -1 10 10 20 30 40 50 60 70 80 90 100 0 0-3 hz -10 10 20 ...bethel/sarsig.pdf · 0 20 40 60 80 100 120 140 160 180 200-50 0 50 6-10 hz 0 20 40 60 80 100 120 140 160 180 200-50 0

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range observations of single scatterer within synthetic aperture

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range observations as function of radar position

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range observations appear as quadratic function

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3COS(Azimuth Phase) = Azimuth Chirp / Squinted, Doppler c.f. != 0

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20range observations of single scatterer within synthetic aperture

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20range observations as function of radar position

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20range observations appear as quadratic function

Page 28: 1 -1 10 10 20 30 40 50 60 70 80 90 100 0 0-3 hz -10 10 20 ...bethel/sarsig.pdf · 0 20 40 60 80 100 120 140 160 180 200-50 0 50 6-10 hz 0 20 40 60 80 100 120 140 160 180 200-50 0

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1150fast vehicle - slow wave propagation - factor x1000

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same graph - longer vehicle trajectory (+/- 20deg)

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big subtended angle +/- 50 deg

now you see it is not really linearjust seems so with small angles