software implementation of digital filters
TRANSCRIPT
MEE 0828
SOFTWARE IMPLEMENTATION OF DIGITAL FILTERS
Satish kumar Are
Manoranjan Reddy Thangalla
Saikrishna Gajjala
This thesis is presented as part of Degree of
Master of Science in Electrical Engineering
Blekinge Institute of Technology
August 2008
Blekinge Institute of Technology School of Engineering Department of Signal Processing Supervisors: Nedelko Grbic Mikael Swartling
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ABSTRACT
This thesis proposes to create a MATLAB GUI (Graphical User Interface) to replace an
existing laboration exercise in signal processing at Blekinge Institute of Technology.
MATLAB is a matrix-based technical computing language widely used throughout the
scientific, engineering and mathematical communities. A GUI provides a graphical interface
between the program and the user, facilitating ease and frequency of use. Development of a
MATLAB GUI for this laboration exercise will benefit the students and increase the
awareness towards designing of digital filters.
The developed software provides an interface between audio recording and playback
hardware and the user when exploring filter design parameters. This software is designed for
analyzing digital filter characteristics such as amplitude, phase and pole/zero locations which
are useful in designing an appropriate filter. This can be achieved by entering arbitrary filter
parameters.
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ACKNOWLEDGMENTS
We would like to express our sincerest thanks and gratitude to Mikael Swartling for being
our mentor on this journey. His guidance, patience and support throughout this project have
been a blessing. We would also like to thank our teacher of signal processing Nedelko Grbic
for providing such a good project and interesting lectures on signal processing. Finally we
would like to thank Mikael Åsman for support and suggestions towards the project.
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Table of Contents
Introduction ............................................................................................................................... 7
Chapter 1: DIGITAL FILTERS ...................................................................................................... 8
1.1 Background ....................................................................................................................... 8
1.2 FIR filters ........................................................................................................................... 9
1.3 Types of windows ........................................................................................................... 10
1.3.1 Rectangular window ................................................................................................ 10
1.3.2 Bartlett window ....................................................................................................... 11
1.3.3 Hanning window ...................................................................................................... 12
1.3.4 Hamming window.................................................................................................... 13
1.3.5 Blackman window ................................................................................................... 14
1.4 Design considerations .................................................................................................... 15
1.5 Observations .................................................................................................................. 16
1.6 IIR filters.......................................................................................................................... 17
1.6.1 Bilinear transformation ........................................................................................... 17
1.6.2 Butterworth approximation .................................................................................... 17
1.6.3 Chebyshev approximation ....................................................................................... 18
1.7 Design considerations .................................................................................................... 19
1.8 Observations .................................................................................................................. 20
Chapter 2 : Developed Software ............................................................................................ 21
2.1 Digital filter software GUI ............................................................................................... 21
2.1.1 Filter selection panel ............................................................................................... 22
2.1.2 Input Selection panel ............................................................................................... 22
2.1.3 Filter specifications panel ........................................................................................ 23
2.2 Digital filter analysis ....................................................................................................... 24
2.2.1 Plot panel ................................................................................................................. 24
2.2.2 Pole/zero plot .......................................................................................................... 25
Conclusion ............................................................................................................................... 26
Appendix .................................................................................................................................. 27
References ............................................................................................................................... 29
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Introduction
Existing problem
For analysis of digital filters, DOS based software was developed years back at Blekinge
Institute of Technology for students of signal processing. However, this software have
drawbacks such as portability, inefficient use of computer resources, less accessibility and
bulk hardware system due to floating point DSP which requires extra hardware for floating
point operations. The developed software has some constraints as it is not user friendly.
Possible solution
With extensive advancements in scientific software, a user friendly graphical user interface
was developed using MATLAB graphical user interface for the analysis of digital filters. This
GUI will overcome the complexities mentioned earlier. The developed software will help the
user to analyze the filters in an efficient manner due to the availability of input signals,
windows, various types of filters such as lowpass, highpass, bandpass, and bandstop filters,
and pole/zero plot with filter coefficients.
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Chapter 1: Digital Filters
1.1 Background
The term ‘filter’ is frequently used in signal processing. A filter is a frequency selective
device that removes unwanted information from the original message signal. Unwanted
signals can be noise or other undesired information. Digital filters are more versatile when
compared to the analog filters in their characteristics such as programming flexibility, ability
to handle both low as well as high frequency signals accurately. Also the hardware
requirement is relatively simple and compact. In real world signals are analog in nature. A
simple signal flow block diagram that explains how the signal is processed to acquire desired
output signal is shown in figure 1.1.
unfiltered sampled digitally filtered analog digitised filtered analog signal signal signal signal
Figure 1.1: Signal flow block diagram.
Analog to digital conversion is an engineering process that enables digital processor to
interact with real world signals. The input to the processor should be properly sampled and
quantized. Sampling and quantization restrict the amount of information a digital signal
contain. In the figure 1.1 an interface is provided between analog signal and the digital signal
processor called analog to digital converter (ADC). The output from ADC is input to the
processor. In applications output from the processor is to be given to user in analog form such
as speech communications, for this an interface is provided from digital domain to the analog
domain. This interface is called digital to analog converter (DAC). Thus the signal is
provided in analog for to the user as shown in figure 1.1. The processor in figure 1.1 can be
anywhere from a large programmable digital computer to a small microprocessor which
contains digital filters.
ADC
DAC
PROCESSOR
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The digital filters are two types based on their impulse response; finite impulse response
(FIR) and infinite impulse response (IIR) filters. FIR filters have same time delay for all
frequencies (linear phase), relatively insensitive to quantization and are always stable. FIR
filters can be designed in different ways, for example window method, frequency sampling
method, weighted least squares method, minimax method and equiripple method. Out of
these methods, the window technique is most conventional method for designing FIR filters.
1.2 FIR filters
A finite impulse response filter of length with input and output is described by
the difference equation
= + − + ⋯ + − +
= −
where is the set of filter coefficients. The transfer function of this filter in domain can be
represented as
=
A window in filter design provides trade off between resolution that is the width of the peak
and spectral leakage that is the amplitude of the tails of desired impulse response. The desired
frequency response specification for linear phase filter is the Fourier transform of the desired
impulse response, and this can be represented as
=
and the inverse as
=
where is the desired frequency response and is the corresponding impulse
response. As is infinite duration, the sample response must be truncated. Truncation is
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performed by multiplying desired sample response with a window function in time domain
which gives sample response of filter represented as
= where is a window function. Various types of windows were used when designing the
FIR filters.
1.3 Types of Windows
1.3.1 Rectangular window
The rectangular window has excellent resolution characteristics for signals of comparable
strength. The rectangular window is defined as
= , !"# $ = 0,1,2, … ) − 1, *+,*-ℎ*#* / The frequency response of the window function is the Fourier transform which, is defined as
0 =
The amplitude response of the rectangular window function is
|0| = |234/||234/| , − ≤ ≤ and the phase response is
7 = 8 − 9 − :, 234 9 : ≥ − 9 − : + , 234 9 : < 0 /
The actual impulse response can be expressed in frequency domain as convolution which
leads to smoothing of . As increases, 0 becomes narrower, thereby reducing
the smoothing effect. In figure 1.2 it is observed that as increases, the main lobe becomes
narrower. However, the amplitude of the side lobes is unaffected. The frequency response of
a lowpass FIR filter designed using rectangular window is shown in figure 1.3 with cutoff
frequency for different window lengths, where cutoff frequency is the characteristic
frequency which determines the type of the filter.
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Figure 1.2: Frequency response for Rectangular window.
Figure 1.3: Lowpass FIR filter designed with Rectangular Window.
1.3.2 Bartlett window
A Bartlett window is a triangular shaped window function. The Bartlett window has higher
side lobe attenuation than the rectangular window. The Bartlett window is defined as
= − = − − = − The frequency response for Bartlett window is shown in figure 1.4 and figure 1.5 shows the
frequency response of a lowpass FIR filter designed using Bartlett window.
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5-150
-100
-50
0
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5
-140
-120
-100
-80
-60
-40
-20
0
20
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
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Figure 1.4: Frequency response for Bartlett window.
Figure 1.5: Lowpass FIR filter designed with Bartlett Window.
1.3.3 Hanning window
The Hanning window is a raised cosine window and can be used to reduce the side lobes
while preserving a good frequency resolution compared to the rectangular window. It is
commonly used as general purpose window for the analysis of continuous signals. The
Hanning window is defined as
= . ? 9 − @A2 − :
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5-150
-100
-50
0
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5
-140
-120
-100
-80
-60
-40
-20
0
20
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
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The frequency response for Hanning window is shown in figure 1.6 and figure 1.7 shows the
frequency response of a lowpass FIR filter designed using Hanning window.
Figure 1.6: Frequency response for Hanning window.
Figure 1.7: Lowpass FIR filter designed with Hanning Window.
1.3.4 Hamming window
The Hamming window is, like the Hanning window, also a raised cosine window. The
Hamming window exhibits similar characteristics to the Hanning window but further
suppress the first side lobe. The Hamming window is defined as
= . ?B − . BC @A2 −
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5-150
-100
-50
0
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5
-140
-120
-100
-80
-60
-40
-20
0
20
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
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The frequency response for Hamming window is shown in figure 1.8 and figure 1.9 shows
the frequency response of a lowpass FIR filter designed using Hamming window.
Figure 1.8: Frequency response for Hamming window.
Figure 1.9: Lowpass FIR filter designed with Hamming Window.
1.3.5 Blackman window
The Blackman window is similar to the Hanning and the Hamming windows. An advantage
with the Blackman window over other windows is that it has better stopband attenuation and
with less passband ripple. The Blackman window is defined as
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5-150
-100
-50
0
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5
-140
-120
-100
-80
-60
-40
-20
0
20
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
15
= . B − . ? @A2 − + . D @A2 B − The frequency response for Blackman window is shown in figure 1.10 and figure 1.11 shows
the frequency response of a lowpass FIR filter designed using Blackman window.
Figure 1.10: Frequency response for Blackman window.
Figure 1.11: Lowpass FIR filter designed with Blackman Window.
1.4 Design considerations
A design consideration when designing digital FIR filter is selecting a window. This can be
done with the help of frequency specifications of the required filter. In general, the frequency
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5-150
-100
-50
0
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 0.45 0.5
-140
-120
-100
-80
-60
-40
-20
0
20
Normalized frequency
Magnitude(d
B)
M=9
M=15
M=21
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specification consists of pass and stopband cutoff frequencies and attenuations. The length of
the filter can be determined by the main lobe width.
Table 1 shows the side lobe attenuation and main lobe width for different windows. Table 2
shows the desired impulse response functions for various filters. Specifically, stopband
attenuation provides for a user to select an appropriate window.
Window Side lobe attenuation Approximate Main lobe width Rectangular -20dB 4F )⁄
Bartlett -27dB 8F )⁄
Hanning -40dB 8F )⁄
Hamming -50dB 8F )⁄
Blackman -70dB 12F )⁄
Table 1: Comparison of main lobe width and side lobe attenuation for different window
types.
Filter Type Desired impulse response I
Lowpass JKF ∙ sin JK P$ − Q) − 12 RS
JK P$ − Q) − 12 RS
Highpass T P$ − 9) − 12 :S − JKF ∙ sin JK P$ − Q) − 12 RSJK P$ − Q) − 12 RS
Bandpass 2 cos WJK P$ − 9) − 12 :SX ∙ JKF ∙ sin JK P$ − Q) − 12 RSJK P$ − Q) − 12 RS
Bandstop T P$ − 9) − 12 :S − 2 cos WJK P$ − 9) − 12 :SX ∙ JKF ∙ sin JK P$ − Q) − 12 RSJK P$ − Q) − 12 RS
Table 2: Desired impulse responses for filter types.
1.5 Observations
From the window frequency response plots shown in the Figures 1.2, 1.4, 1.6, 1.8 and 1.10,
one can observe that as M increases, the main lobe becomes narrower, side lobe amplitudes
remain unaffected but width of the sidelobes decreases. The rectangular window provides
less width in mainlobe and higher sidelobes in contrast with other windows. Using the
window function the ringing effects at the band edges vanishes which results in lower
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sidelobes, thereby increase in the width of the transition band of the lowpass FIR filter as
shown in Figures 1.3, 1.5, 1.7, 1.9 and 1.11.
1.6 IIR filters
Impulse response functions of IIR filters are non-zero over an infinite length of time. IIR
filters can be described using a difference equation as
= Y
Y − Y − Z[
− where Y and Z are the filter coefficients. The transfer function of IIR filters can be
expressed as
= ∑ YY Y + ∑ Z[ These filters can be designed by the bilinear transformation method. These filters are
designed using their analog counterparts rather than discrete time analysis.
1.6.1 Bilinear transformation
The bilinear transformation method is commonly used in designing digital IIR filters to
obtain filter coefficients. As mentioned in section 1.6, digital filters are designed with their
analog counterparts, so it must be transformed into discrete time domain. This transformation
can be done with the bilinear transform.
] = P − + S
1.6.2 Butterworth approximation
The amplitude response of a Butterworth filter is given as
|Ω| = _` + 9 Ω Ωa:[
where [ is order of the filter, Ωa is the passband frequency, Ω is the analog frequency of the
filter specifications, and _ is the maximum value of the amplitude function.
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Figure 1.12
Ω] is the stopband frequency shown in the figure 1.12.The filter order [ can be approximated
as
[ = bAc de` f − g /hibAc 9Ω]Ωa:
where h is the filter parameter which determines the band edge value of |kΩ| and f is
the maximum allowed value for the amplitude function at the stopband edge.
f = |Ω]|lmn
The system transfer function in polynomial form is given by
] = _9 ]Ωa:[ + Z[ 9 ]
Ωa:[ + ⋯ + Z 9 ]Ωa: +
The Butterworth filter coefficients Zo are provided in appendix table A.
1.6.3 Chebyshev approximation
The amplitude response of a Chebyshev filter is given by
|Ω| = _` + h^[ 9 Ω
Ωa:
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Figure 1.13
Figure 1.13 gives us the specifications for order of the Chebyshev filter, where the ripple is
defined as pYaaq = ∙ bAc + h dB and _ is the maximum value of the amplitude
function, ^[ 9 ΩΩa: is the Chebyshev polynomial. The required filter order can be
approximated as
[ =tu]
vwwx
yzzzz` f −
h|~
tu] 9Ω]Ωa:
where h is the filter parameter related to ripple in the passband and f is the maximum
allowed stopband ripple. The system transfer function in polynomial form is given by
] = _ ∙ Z ∙ [ u √ + h [ /9 ]Ωa:[ + Z[ 9 ]
Ωa:[ + ⋯ + Z
The Chebyshev filter coefficients Zo are provided in appendix tables B1, B2, B3 and B4.
1.7 Design considerations
Designing of IIR filters are tricky when compared with FIR filters, here we always consider a
lowpass filter and then transforms the desired filter to and from this lowpass filter. A
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technique called “pre-warping” is used to map digital frequencies into analog frequencies.
The warping frequencies are given by
Ωa = m4 Qa R
Ω] = m4 Q] R
where a and ] angular frequencies of pass and stop bands of digital filters. After “pre
warping” frequency transformation is needed for highpass, bandpass and bandelimination
filters shown in table 3.
Filter Frequency Transformation
Highpass = and =
Bandpass = Ω − Ω and = Ω − Ω , Ω ∙ Ω = Ω ∙ Ω = Ω
Bandelimination = and = , Ω ∙ Ω = Ω ∙ Ω = Ω
Table 3: Transform to frequencies of lowpass filter.
After the frequency transformation, the designed lowpass filter is transformed into the desired
filter type according to the table 4.
LP HP BP BS
]
]
] + Ω]
Ω] + Ω]
Table 4: Transform back to original filter (HP, BP, BS) from lowpass filter.
1.8 Observations
Implementing an IIR filter with certain stopband-attenuation and transition-band
requirements typically requires far fewer filter taps than an FIR filter meeting the same
specifications. This leads to a significant reduction in the computational complexity required
to achieve a given frequency response. However, filter requires feedback to implement an IIR
system, which introduces stability issues. In addition, the filter is of nonlinear phase.
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Chapter 2: Developed software
2.1 Digital Filter Software GUI
A digital filter software GUI is shown in figure 2.1 for design and analysis of digital filters.
The developed filter software GUI consists of the following parts.
Filter selection panel
Input selection panel
Filter specifications panel
A panel for different plots for analysis
A button to display the pole/zero
A button to exit the GUI
Figure 2.1: A simple GUI for design and analysis of digital filters.
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2.1.1 Filter Selection Panel
The user can choose to design and analyze a FIR or IIR digital filter.
2.1.2 Input Selection Panel
The input selection panel consists of settings for the input signal to the digital filter. These
specifications are input signal type, sampling rate and frequency of the signal which are
essential to the analysis of the digital filters.
I. Input
In the Input dropdown list, different types of input signal types can be selected. The signal
types are sine wave, square wave, sawtooth wave and white Gaussian noise. The different
signal types are shown in figure 2.2.
Figure 2.2: The different signal types used in the analysis of digital filters.
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II. Sampling Frequency
The sampling rate is the rate at which the input signal for the filter is sampled. For perfect
reconstruction of a signal the sampling rate should be greater than twice the maximum
frequency of the signal being sampled.
III. Frequency
The frequency determines the number of cycles per unit time of a signal. As the frequency
increases the number of cycles of the input wave also increases. The range of the frequency is
from 0 to Q R − 1 which can be adjusted with the help of a slider and edit box where the
user can directly enter the desired frequency.
2.1.3 Filter specifications panel
I. Filter Type
The user can create lowpass, highpass, bandpass and bandstop. These filters types can be
selected from the dropdown list in the Input selection panel.
II. Filter Order
The filter order mainly determines the width of the transition band. The higher the order, the
narrower is the transition between the passband and stopband, giving a sharper cutoff in the
frequency response. This can be clearly observed in figure 2.3 for orders of 9, 15 and 31.The
transition bandwidth can be improved by increasing the order of the filter. The filter order can
be adjusted between 0 to 31. The filter order can be adjusted by setting the slider or entering
the value in edit box.
Figure 2.3: Plot for different filter orders.
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III. Cut off frequencies
Cutoff frequency is the frequency where the filter is designed to cross over from the passband
to the stopband. The cutoff frequency can be adjusted by setting the values of sliders or
entering the values in the edit box. The cutoff frequencies are in the range from 0 to Q,2 R − 1 . A single cutoff frequency is available for lowpass and highpass filters where as for bandpass
and bandstop two cutoff frequencies are available.
2.2 Digital filter analysis
After designing a digital filter, the filters can be analyzed by selecting different input signals
and examining the filter and filter response in different plots.
2.2.1 Plot Panel
The plot panel consists of three dropdown lists. The dropdown lists presents options for
displaying input and output signals in time domain, linear and logarithmic FFT plots, and
linear and logarithmic filter amplitude responses.
Dropdown list
Time x: shows the input signal in time domain
Time y: shows the filtered signal in time domain
Time x+y: shows the input and output on top of each other in time domain
FFT linear x: shows the amplitude of the FFT of the input signal in linear scale.
FFT linear y: shows the amplitude of the FFT of the output signal in linear scale.
FFT linear x+y: shows the amplitude of the FFT of the input and output signal on top
of each other in linear scale.
FFT logarithmic x: shows the amplitude of the FFT of the input signal in logarithmic
scale.
FFT logarithmic y: shows the amplitude of the FFT of the output signal in logarithmic
scale.
FFT logarithmic x+y: shows the amplitude of the FFT of the input and output signal
on top of each other in logarithmic scale.
FFT linear h: shows the FFT of impulse response in linear scale.
FFT logarithmic h: shows the FFT of impulse response in logarithmic scale.
The FFT is a standard method for decomposition of a signal into harmonic components. It is
the faster version of the Discrete Fourier Transform (DFT). FFT generates the frequency
spectrum for a time domain waveform. The FFT of the impulse response, referred to as the
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frequency response function, completely characterizes the system. Once the system frequency
response is known, one can predict how that system will react to any waveform.
2.2.2 Pole/zero Plot
A pole/zero plot is the graphical representation of the transfer function in the complex Z
plane which helps to convey properties of the system such as stability, causality, minimum
phase and region of convergence.
A linear time invariant system is said to be minimum phase if the system and its inverse are
stable and casual. For a system to be minimum phase all its poles and zeros must be inside
the unit circle. The user can determine whether a digital filter is stable that is output of digital
filter is bounded for all possible bounded inputs. It is known that for IIR filters to be stable is
that all its poles lie inside unit circle where as for FIR filters all its poles lie inside unit circle.
Figure 2.4: A simple pole/zero plot.
A pole/zero plot GUI is shown in figure 2.4. It contains buttons to add, remove and move
filter coefficients and a plot of poles and zeros. The pole/zero plot GUI also contains clear,
restore and update filter coefficients in the main GUI window. In the pole/zero GUI the user
can also pan and zoom the pole/zero plot.
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Conclusion
This Master thesis report presents a software implementation of digital filters using Matlab
GUI in a user friendly environment. The developed software is useful for aspirant students in
designing and analysis of the digital filters. The software consists of radio buttons, pop-up
menus, sliders, edit boxes, axes, push buttons and list boxes all these are placed in different
panels and all are working properly. The evaluated performance using the specific theoretical
filter parameters match the performance with the software. The software is working properly
towards accurate results upon manual testing.
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Appendix
Table A: Coefficients Zo in Butterworth polynomials.
[ Z Z Z ZB Z? ZC Z √2 2 2 B 2.613 3.141 2.613 ? 3.236 5.236 5.236 3.236 C 3.864 7.464 9.141 7.464 3.864 4.494 10.103 14.606 14.606 10.103 4.494 D 5.126 13.138 21.848 25.691 21.848 13.138 5.126
Table B1: Chebyshev filter coefficients Zo.
0.5 # +*¡ = 0.349, ¡ = 0.122.
[ Z Z Z Z ZB Z? ZC Z 2.863 1.516 1.426 0.716 1.535 1.253 B 0.379 1.025 1.717 1.197 ? 0.179 0.752 1.309 1.937 1.172 C 0.095 0.432 1.172 1.589 2.172 1.159 0.045 0.282 0.756 1.648 1.869 2.413 1.151 D 0.024 0.152 0.573 1.148 2.184 2.149 2.657 1.146
Table B2: Chebyshev filter coefficients Zo.
1 # +*¡ = 0.509, ¡ = 0.259.
[ Z Z Z Z ZB Z? ZC Z 1.965 1.102 1.098 0.491 1.238 0.989 B 0.276 0.743 1.454 0.953 ? 0.123 0.580 0.974 1.689 0.937 C 0.069 0.307 0.939 1.202 1.931 0.928 0.031 0.214 0.549 1.357 1.429 2.176 0.923 D 0.017 0.107 0.448 0.447 1.837 1.655 2.423 0.920
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Table B3: Chebyshev filter coefficients Zo.
2 # +*¡ = 0.765, ¡ = 0.585.
[ Z Z Z Z ZB Z? ZC Z 1.307 0.823 0.804 0.327 1.022 0.738 B 0.206 0.517 1.256 0.716 ? 0.082 0.459 0.693 1.499 0.705 C 0.051 0.210 0.771 0.867 1.745 0.701 0.020 0.166 0.383 1.144 1.039 1.994 0.698 D 0.013 0.073 0.359 0.598 1.579 1.212 2.242 0.696
Table B4: Chebyshev filter coefficients Zo.
3 # +*¡ = 0.998, ¡ = 0.995.
[ Z Z Z Z ZB Z? ZC Z 1.002 0.708 0.645 0.251 0.928 0.597 B 0.177 0.405 1.169 0.581 ? 0.063 0.408 0.549 1.415 0.575 C 0.044 0.163 0.699 0.691 1.663 0.571 0.016 0.146 0.300 1.052 0.831 1.911 0.568 D 0.011 0.056 0.321 0.472 1.467 0.972 2.161 0.567
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