Airborne Doppler Radar: Applications, Theory, and Philosophy

Appendix C: Derivation of Parseval Relations

Let f 1( x, y) and f 2( x, y) be two complex valued functions in L 1 so that for a=1 or 2


This condition is sufficient to ensure the convergence of all our integrals. For a = 1 or 2, the two-dimensional Fourier transform pair of these functions is from Eqs. (5.31). [1]



The functions and their transforms then satisfy the Parseval relation


We now note from Eq. (8.8) that


in which g( x, y) is in L 1. Then, with f 1( x, y) = f 2( x, y) = g( x, y) in Eq. (C.4), we have


Further, let


in which both f( x, y) and f x( x, y) are in L 1. Then the Fourier transform of f x( x, y) exists and is


in which F( ? 1, ? 2) is the Fourier transform of f( x, y). Consequently, by letting in Eq. (C.4), we have


Finally, by letting f 1( x, y) = g( x, y) and f 2( x, y) = ?/ ? x g( x, y) in Eq. (C.4) we have


[1] For Eq.(A.2) and Eq. (A.3) to be a Fourier transform pair, it is just required...

UNLIMITED FREE
ACCESS
TO THE WORLD'S BEST IDEAS

SUBMIT
Already a GlobalSpec user? Log in.

This is embarrasing...

An error occurred while processing the form. Please try again in a few minutes.

Customize Your GlobalSpec Experience

Category: Color Meters and Appearance Instruments
Finish!
Privacy Policy

This is embarrasing...

An error occurred while processing the form. Please try again in a few minutes.