

Electronic Warfare and Radar Systems Engineering Handbook  Transforms / Wavelets  

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TRANSFORMS / WAVELETS
Transform Analysis
Signal processing using a transform analysis for calculations is a technique used
to simplify or accelerate problem solution. For example, instead of dividing two large numbers, we might convert them to logarithms, subtract
them, then lookup the antilog to obtain the result. While this may seem a threestep process as opposed to a onestep division, consider that
longhand division of a four digit number by a three digit number, carried out to four places requires three divisions, 34 multiplication*s,
and three subtractions. Computers process additions or subtractions much faster than multiplications or divisions, so transforms are sought
which provide the desired signal processing using these steps.
Fourier Transform
Other types of transforms include
the Fourier transform, which is used to decompose or separate a waveform into a sum of sinusoids of different frequencies. It transforms our
view of a signal from time based to frequency based. Figure 1 depicts how a square wave is formed by summing certain particular sine waves.
The waveform must be continuous, periodic, and almost everywhere differentiable. The Fourier transform of a sequence of rectangular pulses is
a series of sinusoids. The envelope of the amplitude of the coefficients of this series is a waveform with a Sin X/X shape. For the special
case of a single pulse, the Fourier series has an infinite series of sinusoids that are present for the duration of the pulse.
Digital
Sampling of Waveforms
In order to process a signal digitally, we need to sample the signal frequently enough to create a complete “picture” of the signal.
The discrete Fourier transform (DFT) may be used in this regard. Samples are taken at uniform time intervals as shown in Figure 2 and processed.
If the digital information
is multiplied by the Fourier coefficients, a digital filter is created as shown Figure 3. If the sum of the resultant components is zero, the
filter has ignored (notched out) that frequency sample. If the sum is a relatively large number, the filter has passed the signal. With the
single sinusoid shown, there should be only one resultant. (Note that being “zero” and relatively large may just mean below or above the filter*s
cutoff threshold) Figure 4 depicts the process pictorially: The vectors in the figure just happen to be pointing in a cardinal
direction because the strobe frequencies are all multiples of the vector (phasor) rotation rate, but that is not normally the case. Usually
the vectors will point in a number of different directions, with a resultant in some direction other than straight up. In addition,
sampling normally has to taken at or above twice the rate of interest (also known as the Nyquist rate), otherwise ambiguous results may be obtained.
Figure 4. Phasor Representation
Fast Fourier Transforms
One problem with this type of processing is the large number
of additions, subtractions, and multiplications which are required to reconstruct the output waveform. The Fast Fourier transform (FFT) was
developed to reduce this problem. It recognizes that because the filter coefficients are sine and cosine waves, they are symmetrical about 90,
180, 270, and 360 degrees. They also have a number of coefficients equal either to one or zero, and duplicate coefficients from filter to filter
in a multibank arrangement. By waiting for all of the inputs for the bank to be received, adding together those inputs for which coefficients
are the same before performing multiplications, and separately summing those combinations of inputs and products which are common to more than
one filter, the required amount of computing may be cut drastically.
 The number of computations for a DFT is on the order of N squared.
 The number of computations for a FFT when N is a power of two is on the order of N log2 N.
For example, in an eight filter bank, a DFT would require 512 computations, while an FFT would only require 56, significantly speeding up
processing time.
Windowed Fourier Transform
The Fourier transform is continuous, so a windowed Fourier transform (WFT) is used to analyze nonperiodic signals as shown in Figure
5. With the WFT, the signal is divided into sections (one such section is shown in Figure 5) and each section is analyzed for frequency content.
If the signal has sharp transitions, the input data is windowed so that the sections converge to zero at the endpoints. Because a single window
is used for all frequencies in the WFT, the resolution of the analysis is the same (equally spaced) at all locations in the timefrequency domain.
The FFT works well for signals with smooth or uniform frequencies, but it has been found that other transforms work better with signals
having pulse type characteristics, timevarying (nonstationary) frequencies, or odd shapes.
The FFT also does not distinguish sequence
or timing information. For example, if a signal has two frequencies (a high followed by a low or vice versa), the Fourier transform only reveals
the frequencies and relative amplitude, not the order in which they occurred. So Fourier analysis works well with stationary, continuous, periodic,
differentiable signals, but other methods are needed to deal with nonperiodic or nonstationary signals.
Wavelet
Transform
The Wavelet transform has been evolving for some time. Mathematicians theorized its use in the early 1900's. While the
Fourier transform deals with transforming the time domain components to frequency domain and frequency analysis, the wavelet transform deals
with scale analysis, that is, by creating mathematical structures that provide varying time/frequency/amplitude slices for analysis. This transform
is a portion (one or a few cycles) of a complete waveform, hence the term wavelet. The wavelet transform has the ability to identify frequency
(or scale) components, simultaneously with their location(s) in time. Additionally, computations are directly proportional to the length of
the input signal. They require only N multiplications (times a small constant) to convert the waveform. For the previous eight filter bank example,
this would be about twenty calculations, vice 56 for the FFT. In wavelet analysis, the scale that one uses in looking at data plays
a special role. Wavelet algorithms process data at different scales or resolutions. If we look at a signal with a large "window," we would notice
gross features. Similarly, if we look at a signal with a small "window," we would notice small discontinuities as shown in Figure 6. The result
in wavelet analysis is to "see the forest and the trees." A way to achieve this is to have short highfrequency fine scale functions and long
lowfrequency ones. This approach is known as multiresolution analysis.
For many decades, scientists have wanted more appropriate functions
than the sines and cosines (base functions) which comprise Fourier analysis, to approximate choppy signals. (Although Walsh transforms work
if the waveform is periodic and stationary). By their definition, sine and cosine functions are nonlocal (and stretch out to infinity), and
therefore do a very poor job in approximating sharp spikes. But with wavelet analysis, we can use approximating functions that are contained
neatly in finite (time/frequency) domains. Wavelets are wellsuited for approximating data with sharp discontinuities.
The wavelet analysis
procedure is to adopt a wavelet prototype function, called an "analyzing wavelet" or "mother wavelet." Temporal analysis is performed with a
contracted, highfrequency version of the prototype wavelet, while frequency analysis is performed with a dilated, lowfrequency version of
the prototype wavelet. Because the original signal or function can be represented in terms of a wavelet expansion (using coefficients in a linear
combination of the wavelet functions), data operations can be performed using just the corresponding wavelet coefficients as shown in Figure
7.
If one further
chooses the best wavelets adapted to the data, or truncates the coefficients below some given threshold, the data is sparsely represented. This
"sparse coding" makes wavelets an excellent tool in the field of data compression. For instance, the FBI uses wavelet coding to store fingerprints.
Hence, the concept of wavelets is to look at a signal at various scales and analyze it with various resolutions.
Analyzing Wavelet Functions
Fourier transforms deal with just two basis functions (sine and
cosine), while there are an infinite number of wavelet basis functions. The freedom of the analyzing wavelet is a major difference between the
two types of analyses and is important in determining the results of the analysis. The “wrong” wavelet may be no better (or even far worse than)
than the Fourier analysis. A successful application presupposes some expertise on the part of the user. Some prior knowledge about the signal
must generally be known in order to select the most suitable distribution and adapt the parameters to the signal. Some of the more common ones
are shown in Figure 8. There are several wavelets in each family, and they may look different than those shown. Somewhat longer in duration
than these functions, but significantly shorter than infinite sinusoids is the cosine packet shown in Figure 9.
Wavelet Comparison With Fourier Analysis
While a typical Fourier transform provides frequency content information for samples
within a given time interval, a perfect wavelet transform records the start of one frequency (or event), then the start of a second event, with
amplitude added to or subtracted from, the base event.
Example 1.
Wavelets are especially useful in analyzing
transients or timevarying signals. The input signal shown in Figure 9 consists of a sinusoid whose frequency changes in stepped increments
over time. The power of the spectrum is also shown. Classical Fourier analysis will resolve the frequencies but cannot provide any information
about the times at which each occurs. Wavelets provide an efficient means of analyzing the input signal so that frequencies and the times at
which they occur can be resolved. Wavelets have finite duration and must also satisfy additional properties beyond those normally associated
with standard windows used with Fourier analysis. The result after the wavelet transform is applied is the plot shown in the lower right. The
wavelet analysis correctly resolves each of the frequencies and the time when it occurs. A series of wavelets is used in example 2.
Example 2. Figure 10 shows the input of a clean signal, and one with noise. It also shows the output
of a number of “filters” with each signal. A 6 dB S/N improvement can be seen from the d4 output. (Recall from Section 4.3 that 6 dB corresponds
to doubling of detection range.) In the filter cascade, the HPFs and LPFs are the same at each level. The wavelet shape is related to the HPF
and LPF in that it is the “impulse response” of an infinite cascade of the HPFs and LPFs. Different wavelets have different HPFs and LPFs. As
a result of decimating by 2, the number of output samples equals the number of input samples.
Wavelet Applications Some fields that are
making use of wavelets are: astronomy, acoustics, nuclear engineering, signal and image processing (including fingerprinting), neurophysiology,
music, magnetic resonance imaging, speech discrimination, optics, fractals, turbulence, earthquakeprediction, radar, human vision, and pure
mathematics applications. See October 1996 IEEE Spectrum article entitled “Wavelet Analysis”, by Bruce, Donoho, and Gao.
Table of Contents
for Electronics Warfare and Radar Engineering Handbook
Introduction 
Abbreviations  Decibel  Duty
Cycle  Doppler Shift  Radar Horizon / Line
of Sight  Propagation Time / Resolution  Modulation
 Transforms / Wavelets  Antenna Introduction
/ Basics  Polarization  Radiation Patterns 
Frequency / Phase Effects of Antennas 
Antenna Near Field  Radiation Hazards 
Power Density  OneWay Radar Equation / RF Propagation
 TwoWay Radar Equation (Monostatic) 
Alternate TwoWay Radar Equation 
TwoWay Radar Equation (Bistatic) 
Jamming to Signal (J/S) Ratio  Constant Power [Saturated] Jamming
 Support Jamming  Radar Cross Section (RCS) 
Emission Control (EMCON)  RF Atmospheric
Absorption / Ducting  Receiver Sensitivity / Noise 
Receiver Types and Characteristics 
General Radar Display Types 
IFF  Identification  Friend or Foe  Receiver
Tests  Signal Sorting Methods and Direction Finding 
Voltage Standing Wave Ratio (VSWR) / Reflection Coefficient / Return
Loss / Mismatch Loss  Microwave Coaxial Connectors 
Power Dividers/Combiner and Directional Couplers 
Attenuators / Filters / DC Blocks 
Terminations / Dummy Loads  Circulators
and Diplexers  Mixers and Frequency Discriminators 
Detectors  Microwave Measurements 
Microwave Waveguides and Coaxial Cable 
ElectroOptics  Laser Safety 
Mach Number and Airspeed vs. Altitude Mach Number 
EMP/ Aircraft Dimensions  Data Busses  RS232 Interface
 RS422 Balanced Voltage Interface  RS485 Interface 
IEEE488 Interface Bus (HPIB/GPIB)  MILSTD1553 &
1773 Data Bus  This HTML version may be printed but not reproduced on websites.



