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Electromagnetic Sensing for Space-borne Imaging. Lecture 7 Beam Steering, Optimal Beam Forming. Beam Steering: Consider the 1-D Array Example, But let the weights be more general. Beam Steering: Consider the 1-D Array Example, But let the weights be more general.
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Electromagnetic Sensing for Space-borne Imaging Lecture 7Beam Steering, Optimal Beam Forming
Beam Steering: Consider the 1-D Array Example, But let the weights be more general
Beam Steering: Consider the 1-D Array Example, But let the weights be more general
Let’s construct a reasonably general 2-D Array Model yP m n D xP Square Array, N apertures on a side
yQ xQ What does the ground plane power distribution look like? • The small spots are potential power reception areas (covered by rectennas). We would like these to be small. • The big circle is the maximum coverage area. We would like this to be large enough to service ~ 10 reception stations.
How to get the desired power distribution on the ground • Assumptions: • The phased array geometry and dimensions are given. • We want a specific field amplitude distribution on the ground. Denote this by • Question: What phased array gains will produce the best possible approximation to in the sense that we minimize: • Where and have the same total power
“The old RF guys never died. They just phased array” - Anon. Gain Time delay 4 1 3 2 5 Assumption: The individual transmitter apertures all have immediate neighbors with spacing
L2 Space of Lebesgue Integrable Functions • “L” for Henri Lebesgue, superscript “2” to denote a generalization of the vector 2-norm • Generally, a finite or infinite dimensional, linear vector space • An inner product is defined • The inner product induces the norm • The specific L2space we use is the space of all square-integrable, complex-valued functions of two variables. For an f(x,y) in this space:
There is another way to suppress side beams- Randomize the transmitter locations! yP D xP