Signal Processing: A Mathematical Approach

Part Eleven: More Applications

Chapter List

Chapter 56: The Wave Equation
Chapter 57: Array Processing
Chapter 58: Matched Field Processing
Chapter 59: Transmission Tomography
Chapter 60: Scattering
Chapter 61: A Simple Model for Remote Sensing
Chapter 62: Poisson Mixtures
Chapter 63: Hyperspectral Imaging

In this chapter and the next, we demonstrate how the problem of Fourier-transform estimation from sampled data arises in the processing of measurements obtained by sampling electromagnetic- or acoustic-field fluctuations, as in radar or sonar.

In many areas of remote sensing, what we measure are the fluctuations in time of an electromagnetic or acoustic field. Such fields are described mathematically as solutions of certain partial differential equations, such as the wave equation. A function u( x, y, z, t) is said to satisfy the three- dimensional wave equation if


where u tt denotes the second partial derivative of u with respect to the time variable t twice and c > 0 is the (constant) speed of propagation. More complicated versions of the wave equation permit the speed of propagation c to vary with the spatial variables x, y, z, but we shall not consider that here.

We use the method of separation of variables at this point, to get some idea about the nature of solutions of the wave equation. Assume, for the moment, that the solution u( t, x, y, z) has the simple form


Inserting this separated form into the wave equation, we get


or


The function...

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