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The Uncertainty Principle

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Part of the book series: Applied Physics and Engineering ((APPLIED PHYS,volume 4))

Abstract

It has thus far been assumed that the received signal is reflected from a stationary target so that the carrier frequency of the transmitted and reflected signals coincide. The general case will now be considered. Assume that the signal is reflected from a target whose range is r0, and whose range rate is v0. Thus the reflected signal is delayed by the time t0 = 2r0/c and acquires a Doppler shift of Q = (2v0/c) ω0:

$$ {s_{1}}\left( t \right) = s\left( {t - {t_{0}}} \right){e^{{j\Omega \left( {t - {t_{0}}} \right)}}} $$

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Ernest Jacobs

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© 1968 Springer-Verlag New York Inc.

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Vakman, D.E. (1968). The Uncertainty Principle. In: Jacobs, E. (eds) Sophisticated Signals and the Uncertainty Principle in Radar. Applied Physics and Engineering, vol 4. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-88213-5_2

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  • DOI: https://doi.org/10.1007/978-3-642-88213-5_2

  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-642-88215-9

  • Online ISBN: 978-3-642-88213-5

  • eBook Packages: Springer Book Archive

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