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Extrapolation of Wideband Responses from Resonant Antennas
using Early-Time and Low-Frequency Data
J. Michael Frye and Dr. Anthony Q. Martin
Abstract
Response Representation
Obtaining a wideband response from a resonant
antenna using traditional electromagnetic numerical
methods is often very computationally demanding. A
technique is presented which accurately extrapolates
the complete response using only early-time and lowfrequency data, which can be obtained relatively easily.
The response is represented as a summation of N
orthogonal polynomials and M damped sinusoids.
Damped sinusoids are utilized to efficiently represent
the effects of resonances in the response. A genetic
algorithm (GA) is used to select all required
parameters for stable and accurate results.
Numerical Results
Time and freq. response represented by two summations:
E-Shaped Patch Antenna
N weighted orthogonal polynomials: n t , n f
Associate Hermite polynomials used
M damped sinusoids: gm t , Gm f
Represent “resonant” behavior of response
Amplitude, decay factor, and resonant freq. define each pair
N 1
M 1
n 0
m0
x t xˆ t a n n t / l1 g m t
N 1
M 1
n 0
m 0
Extrapolation of Driving-Point Current Response
X f Xˆ f a n n f / l2 Gm f
Applications
Rapid numerical analysis of resonant antennas over
an ultra-wide frequency band
Tool for the design and analysis of wideband, multiband, or switched antennas
xˆ t , Xˆ f
Extrapolation Approach
Early-time and low-freq. data used to extrapolate
complete time & freq. response (late-time, high-freq.)
are the extrapolated versions of x t , X f
Single set of N polynomial weighting coefficients: a n
Determined from matrix eq. using only early-time/low-freq. data
Damped sinusoid parameters found from response data
Aid in optimization of antenna designs which meet
performance goals for multiple applications
GA-Based Parameter Selection
Represents possible parameter combinations as chromosomes
x t : time - domain response
Finds optimal solution by evaluating ‘fitness’ of potential solutions
Minimize difference between actual and extrapolated responses:
ˆ
X
X
ˆ
1 xx
E
,
2
x
X
X f : freq.- domain response
Partition into early/late-time and low/high-freq data:
X f X LF , X HF
Highly resonant: cavity
modes, slot and wire
resonances
Differentiated Gaussian
pulse voltage excitation
up to 15 GHz
Extrapolated response:
driving-point current
due to pulse
Genetic algorithm (GA) optimization is utilized
Low-freq. data contains late-time information
x
xi
Data to left of vertical dashed line is known (early-time/low-freq.)
Data to right is extrapolated (late-time/high-freq.)
Accurate extrapolation with 6% of time data and 25% of freq. data
N=32 (orthogonal polynomials), M=9 (damped sinusoids)
Cavity-Backed Slot Antenna with Monopole
Parameters must be carefully selected for stable/accurate results
Global search technique inspired by evolutionary biology concepts
Computationally intensive data (late-time, high –freq.)
is extrapolated rather than directly computed.
Accurately characterize resonances of response
Early-time data contains high-freq. information
x t xET , xLT
Dual-band (1.9 GHz & 2.4 GHz)
Designed for wireless
communications applications
Differentiated Gaussian pulse
voltage excitation up to 4 GHz
Extrapolated response:
driving-point current due
to pulse
Represent “transient” behavior of response
2
i
Extrapolation of Driving-Point Current Response
E cannot be directly minimized in practice because it requires
complete knowledge of the response (which must be extrapolated)
Approximate E using only early-time/low-freq data:
1
ˆ
E
2
xET xˆ ET IFFT Xˆ
xET
LT
xˆ LT
X LF
Xˆ LF FFT xˆ HF Xˆ HF
X LF
By minimizing Ê , all necessary extrapolation parameters can be
reliably selected to yield an accurate extrapolation
Vertical dash line indicates point of extrapolation
Accurate extrapolation with 2.5% of time data and 25% of freq. data
N=484 (orthogonal polynomials), M=44 (damped sinusoids)