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UNIT-I
DISCRETE FOURIER TRANSFORM
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Syllabus
• Discrete Signals and Systems- A Review• Introduction to DFT • Properties of DFT• Circular Convolution• Filtering methods based on DFT• FFT Algorithms • Decimation in time Algorithms,• Decimation in frequency Algorithms • Use of FFT in Linear Filtering.
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Signal Processing• Humans are the most advanced signal processors
– speech and pattern recognition, speech synthesis,…• We encounter many types of signals in various applications
– Electrical signals: voltage, current, magnetic and electric fields,…– Mechanical signals: velocity, force, displacement,…– Acoustic signals: sound, vibration,…– Other signals: pressure, temperature,…
• Most real-world signals are analog– They are continuous in time and amplitude– Convert to voltage or currents using sensors and transducers
• Analog circuits process these signals using– Resistors, Capacitors, Inductors, Amplifiers,…
• Analog signal processing examples– Audio processing in FM radios– Video processing in traditional TV sets
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Limitations of Analog Signal Processing• Accuracy limitations due to
– Component tolerances– Undesired nonlinearities
• Limited repeatability due to– Tolerances– Changes in environmental conditions
• Temperature• Vibration
• Sensitivity to electrical noise• Limited dynamic range for voltage and currents• Inflexibility to changes • Difficulty of implementing certain operations
– Nonlinear operations– Time-varying operations
• Difficulty of storing information
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Digital Signal Processing• Represent signals by a sequence of numbers
– Sampling or analog-to-digital conversions
• Perform processing on these numbers with a digital processor
– Digital signal processing
• Reconstruct analog signal from processed numbers
– Reconstruction or digital-to-analog conversion
A/D DSP D/Aanalogsignal
analogsignal
digital signal
digital signal
• Analog input – analog output – Digital recording of music
• Analog input – digital output– Touch tone phone dialing
• Digital input – analog output– Text to speech
• Digital input – digital output– Compression of a file on computer
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Pros and Cons of Digital Signal Processing
• Pros– Accuracy can be controlled by choosing word length– Repeatable– Sensitivity to electrical noise is minimal– Dynamic range can be controlled using floating point numbers– Flexibility can be achieved with software implementations– Non-linear and time-varying operations are easier to implement – Digital storage is cheap– Digital information can be encrypted for security– Price/performance and reduced time-to-market
• Cons– Sampling causes loss of information– A/D and D/A requires mixed-signal hardware– Limited speed of processors– Quantization and round-off errors
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Discrete Signals and Systems
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Discrete-Time Signals: Sequences• Discrete-time signals are represented by sequence of numbers
– The nth number in the sequence is represented with x[n]
• Often times sequences are obtained by sampling of continuous-time signals
– In this case x[n] is value of the analog signal at xc(nT)
– Where T is the sampling period
0 20 40 60 80 100-10
0
10
t (ms)
0 10 20 30 40 50-10
0
10
n (samples)
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Basic Sequences and Operations• Delaying (Shifting) a sequence
• Unit sample (impulse) sequence
• Unit step sequence
• Exponential sequences
]nn[x]n[y o
0n1
0n0]n[
0n1
0n0]n[u
nA]n[x
-10 -5 0 5 100
0.5
1
1.5
-10 -5 0 5 100
0.5
1
1.5
-10 -5 0 5 100
0.5
1
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Sinusoidal Sequences• Important class of sequences
• An exponential sequence with complex
• x[n] is a sum of weighted sinusoids• Different from continuous-time, discrete-time sinusoids
– Have ambiguity of 2k in frequency
– Are not necessary periodic with 2/o
ncosnx o
jj eAA and e o
nsinAjncosAnx
eAeeAAnx
o
n
o
n
njnnjnjn oo
ncosnk2cos oo
integer an is k2
N if only Nncosncoso
ooo
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Discrete-Time Systems• Discrete-Time Sequence is a mathematical operation that maps a given
input sequence x[n] into an output sequence y[n]
• Example Discrete-Time Systems– Moving (Running) Average
– Maximum
– Ideal Delay System
]}n[x{T]n[y T{.}x[n] y[n]
]3n[x]2n[x]1n[x]n[x]n[y
]2n[x],1n[x],n[xmax]n[y
]nn[x]n[y o
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Memoryless System• Memoryless System
– A system is memoryless if the output y[n] at every value of n depends only on the input x[n] at the same value of n
• Example Memoryless Systems– Square
– Sign
• Counter Example– Ideal Delay System
2]n[x]n[y
]n[xsign]n[y
]nn[x]n[y o
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Linear Systems• Linear System: A system is linear if and only if
• Examples– Ideal Delay System
(scaling) ]n[xaT]n[axT
and
y)(additivit ]n[xT]n[xT]}n[x]n[x{T 2121
]nn[x]n[y o
]nn[ax]n[xaT
]nn[ax]n[axT
]nn[x]nn[x]n[xT]}n[x{T
]nn[x]nn[x]}n[x]n[x{T
o1
o1
o2o112
o2o121
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Time-Invariant Systems• Time-Invariant (shift-invariant) Systems
– A time shift at the input causes corresponding time-shift at output
• Example– Square
• Counter Example– Compressor System
]nn[xT]nn[y]}n[x{T]n[y oo
2]n[x]n[y
2oo
2o1
]nn[xn-ny gives output the Delay
]nn[xny is output the input the Delay
]Mn[x]n[y
oo
o1
nnMxn-ny gives output the Delay
]nMn[xny is output the input the Delay
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Causal System• Causality
– A system is causal it’s output is a function of only the current and previous samples
• Examples– Backward Difference
• Counter Example– Forward Difference
]n[x]1n[x]n[y
]1n[x]n[x]n[y
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Stable System• Stability (in the sense of bounded-input bounded-output BIBO)
– A system is stable if and only if every bounded input produces a bounded output
• Example– Square
• Counter Example– Log
yx B]n[y B]n[x
2]n[x]n[y
2x
x
B]n[y by bounded is output
B]n[x by bounded is input if
]n[xlog]n[y 10
nxlog0y 0nxfor bounded not output
B]n[x by bounded is input if even
10
x
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DFS,DTFT & DFT
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Fourier Transform of continuous time signals
dtetxtxFTfX ftj 2)()()(
dfefXfXIFTtx ftj 2)()()(
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Linear Time Invariant (LTI) Systems and z-Transform
][nx ][ny][nh
If the system is LTI we compute the output with the convolution:
m
mnxmhnxnhny ][][][*][][
If the impulse response has a finite duration, the system is called FIR (Finite Impulse Response):
][][...]1[]1[][]0[][ NnxNhnxhnxhny
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n
nznxnxZzX ][][)(
Z-Transform
Facts:
)()()( zXzHzY
][nx ][ny)(zH
Frequency Response of a filter:
fjezzHfH 2)()(
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Frequency-Domain Properties
Time
Continuous
Discrete
PeriodicityPeriodic Aperiodic
Fourier SeriesFourier Series Continuous-TimeFourier Transform
Continuous-TimeFourier Transform
DFTDFT
DurationFinite Infinite
Discrete-TimeFourier Transformand z-Transform
Discrete-TimeFourier Transformand z-Transform
Discrete &
Aperiodic
Discrete &
Aperiodic
Continuous &
Aperiodic
Continuous &
Aperiodic
Continuous &
Periodic (2)
Continuous &
Periodic (2)
Discrete &
Periodic
Discrete &
Periodic
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Signal Processing Methods
Time
Continuous
Discrete
PeriodicityPeriodic Aperiodic
Fourier SeriesFourier Series Continuous-TimeFourier Transform
Continuous-TimeFourier Transform
DFSDFS
DurationFinite Infinite
Discrete-TimeFourier Transformand z-Transform
Discrete-TimeFourier Transformand z-Transform
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The Four Fourier Methods
28
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Relations Among Fourier Methods
29
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The Family of Fourier Transform
Aperiodic-Continuous - Fourier Transform
dejXtx
dtetxjX
tj
tj
)(2
1)(
)()(
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The Family of Fourier Transform
Periodic-Continuous - Fourier Series
k
tjk
T
T
tjk
ejkXtx
dtetxT
jkX
0
0
0
0
)()(
)(1
)(
0
2
20
0
00
22
TF
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The Family of Fourier Transform
Periodic-Discrete - DFS (DFT)
1
0
2
1
0
2
)(1
)(
)()(
N
k
nkN
j
N
n
nkN
j
ekXN
nx
enxkX
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Introduction
The Discrete Fourier Transform (DFT)
The DFS provided us a mechanism for numerically computing the discrete-time Fourier transform. But most of the signals in practice are not periodic. They are likely to be of finite length.
Theoretically, we can take care of this problem by defining a periodic signal whose primary shape is that of the finite length signal and then using the DFS on this periodic signal.
Practically, we define a new transform called the Discrete Fourier Transform, which is the primary period of the DFS.
This DFT is the ultimate numerically computable Fourier transform for arbitrary finite length sequences.
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Finite-length sequence & periodic sequence
The Discrete Fourier Transform (DFT)
)(nx Finite-length sequence that has N samples
)(~ nx periodic sequence with the period of N
)()(~)(
,0
10 ),(~)(
nRnxnx
elsewhere
Nnnxnx
N
))(()(~
)()(~
N
r
nxnx
rNnxnx
Window operation
Periodic extension
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The Family of Fourier Transform
Aperiodic-Discrete - DTFT
deeXnx
enxeX
njj
n
njj
)(2
1)(
)()(
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DFT and IDFT
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IDFT
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The definition of DFT
The Discrete Fourier Transform (DFT)
10 ,)(1
)]([IDFT)(
10 ,)()]([DFT)(
1
0
1
0
NnWkXN
kXnx
NkWnxnxkX
N
n
nkN
N
n
nkN
)()(~)()(1
)(
)()(~
)()()(
1
0
1
0
nRnxnRWkXN
nx
kRkXkRWnxkX
N
N
nN
nkN
N
N
nN
nkN
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Twiddle factor
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Relationship of DFT to other transforms
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Problems on DFT
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Example of DFT
• Find X[k]
– We know k=1,.., 7; N=8
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Example of DFT
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Example of DFT
Time shift Property of DFT
Polar plot for
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Example of DFT
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Example of DFT
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Example of DFT
Summation for X[k]
Using the shift property!
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Example of DFT
Summation for X[k]
Using the shift property!
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Example of IDFT
Remember:
![Page 52: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/52.jpg)
Example of IDFT
Remember:
![Page 53: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/53.jpg)
Problems on DFT
![Page 54: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/54.jpg)
Problems on DFT
![Page 55: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/55.jpg)
![Page 56: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/56.jpg)
![Page 57: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/57.jpg)
![Page 58: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/58.jpg)
Circular shift of a sequence
![Page 59: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/59.jpg)
![Page 60: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/60.jpg)
![Page 61: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/61.jpg)
![Page 62: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/62.jpg)
The Properties of DFT
Linearity
)()()]()([DFT 2121 kbXkaXnbxnax N3-point DFT, N3=max(N1,N2)
Circular shift of a sequence
)()]())(([DFT kXWnRmnx kmNNN
)())(()]([DFT kRlkXnxW NNnl
N Circular shift in the frequency domain
![Page 63: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/63.jpg)
The Properties of DFT
The sum of a sequence
1
00
1
00
)()()(N
nk
N
n
nkNk
nxWnxkX
The first sample of sequence
1
0
)(1
)0(N
k
kXN
x
)())(()]([
)()]([
kRkNNxnXDFT
kXnxDFT
NN
![Page 64: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/64.jpg)
The Properties of DFT
Circular convolution
)( )()())(()(
)())(()()( )(
12
1
012
1
02121
nxnxnRmnxmx
nRmnxmxnxnx
N
N
mN
N
N
mN
N
N
)()()]( )([DFT 2121 kXkXnxnx N
)( )(1
)]()([DFT 2121 kXkXN
nxnx N
Multiplication
![Page 65: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/65.jpg)
The Properties of DFT
Circular convolution
)( )()())(()(
)())(()()( )(
12
1
012
1
02121
nxnxnRmnxmx
nRmnxmxnxnx
N
N
mN
N
N
mN
N
N
)()()]( )([DFT 2121 kXkXnxnx N
)( )(1
)]()([DFT 2121 kXkXN
nxnx N
Multiplication
![Page 66: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/66.jpg)
The Properties of DFT
Circular correlation
nn
xy nymnxmnynxmr )(*)()(*)()(
Circular correlation
)()(*))((
)())((*)()(
1
0
1
0
mRnymnx
mRmnynxmr
N
N
nN
N
N
nNxy
Linear correlation
![Page 67: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/67.jpg)
The Properties of DFT
)()(*))((
)())((*)(
)]([IDFT)(
)()()(
1
0
1
0
*
mRnymnx
mRmnynx
kRmrthen
kYkXkRif
N
N
nN
N
N
nN
xyxy
xy
![Page 68: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/68.jpg)
The Properties of DFT
Parseval’s theorem
1
0
*1
0
* )()(1
)()(N
k
N
n
kYkXN
nynx
1
0
21
0
2
1
0
*1
0
*
)(1
)(
)()(1
)()(then
)()( let
N
k
N
n
N
k
N
n
kXN
nx
kXkXN
nxnx
nynx
![Page 69: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/69.jpg)
The Properties of DFT
Conjugate symmetry properties of DFT
and)(nxep )(nxopLet be a N-point sequence)(nx Nnxnx ))(()(~
]))(())(([2
1)](~)(~[
2
1)(~
]))(())(([2
1)](~)(~[
2
1)(~
NNo
NNe
nNxnxnxnxnx
nNxnxnxnxnx
It can be proved that
)(~)(~)(~)(~
*
*
nxnx
nxnx
oo
ee
![Page 70: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/70.jpg)
The Properties of DFT
)())(())((2
1
)()(~)(
)())(())((2
1
)()(~)(
nRnNxnx
nRnxnx
nRnNxnx
nRnxnx
NNN
Noop
NNN
Neep
Circular conjugate symmetriccomponent
Circular conjugate antisymmetriccomponent
![Page 71: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/71.jpg)
The Properties of DFT
)()()( nxnxnx opep
)())(()(
)())(()(*
*
nRnNxnx
nRnNxnx
NNopop
NNepep
![Page 72: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/72.jpg)
The Properties of DFT
)()()( kXkXkX opep
)())(()(
)())(()(*
*
kRkNXkX
kRkNXkX
NNopop
NNepep
and)(kX ep )(kX op
![Page 73: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/73.jpg)
The Properties of DFT
)]())((Im[)](Im[
)]())((Re[)](Re[
kRkNXkX
kRkNXkX
NNepep
NNepep
)]())((Im[)](Im[
)]())((Re[)](Re[
kRkNXkX
kRkNXkX
NNopop
NNopop
![Page 74: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/74.jpg)
The Properties of DFT
)())(()(then
)())(()( if
kRkNXkX
nRnNxnx
NN
NN
Circular even sequences
Circular odd sequences
)())(()(then
)())(()( if
kRkNXkX
nRnNxnx
NN
NN
![Page 75: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/75.jpg)
Circular convolution in Time domain
![Page 76: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/76.jpg)
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![Page 78: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/78.jpg)
Circular convolution
![Page 79: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/79.jpg)
![Page 80: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/80.jpg)
![Page 81: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/81.jpg)
![Page 82: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/82.jpg)
![Page 83: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/83.jpg)
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Circular convolution-Example
![Page 85: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/85.jpg)
85
x1(n)=(1,2,3) and x2(n)=(4,5,6).
One sequence is distributed clockwise and
the other counterclockwise and the shift of the inner circle is clockwise.
1
23
6
54
*
+
* *
++
=6+10+12=28
1st term
1
23
4
65
*
+
* *
++
=4+12+15=31
2st term
![Page 86: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/86.jpg)
86
1
23
5
46
*
+
* *
++
=5+8+18=31
3rd term
x1(n)* x2(n)=(1,2,3)*(4,5,6)=(18,31,31).
We have the same symmetry as before
˜ y (n) ˜ x 1 (k) ˜ x 2 (n k)k0
N 1
˜ y (n) ˜ x 2(k) ˜ x 1(n k)k0
N 1
![Page 87: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/87.jpg)
Cirular convolution-Matrix method
![Page 88: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/88.jpg)
Circular convolution property
![Page 89: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/89.jpg)
![Page 90: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/90.jpg)
![Page 91: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/91.jpg)
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Use of DFT in linear filtering
1
0
][][][L
k
knhkxny
DFT- based filtering always performs circular convolution.But by zero padding adequetly,Circular convoltion can yield the same result.
where n=0.....(L+M-1)-1
![Page 94: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/94.jpg)
Linear convolution using DFT
1][][)( 21 LLNoflen g thtonhan dnxpa dd in gz er oa
![Page 95: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/95.jpg)
][*][][)( nhnxnya
(2) calculate linear convolution by circular convolution
1][][)( 21 LLNoflen g thtonhan dnxpa dd in gz er oa
1][][)( 21 LLNoflen g thtonhan dnxpa dd in gz er oa
(1)calculate N point circular convolution by linear convolution
(3) calculate linear convolution by DFT
][][][)]([)( nRrNnynhNnxb N
r
][)] ([][][)( nhNnxnhnxb
][][in t)( nhandnxo fD FTspoNb
][)]([][*][
]}[][{][)]([)(
nhNnxnhnx
kHkXIDFTnhNnxc
LINEAR & CIRCULAR CONVOLUTION
![Page 96: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/96.jpg)
Example:Cir.conv
![Page 97: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/97.jpg)
Circular conv
![Page 98: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/98.jpg)
FAST FOURIER TRANSFORM
![Page 99: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/99.jpg)
Discrete Fourier Transform
• The DFT pair was given as
• Baseline for computational complexity:
– Each DFT coefficient requires
• N complex multiplications
• N-1 complex additions
– All N DFT coefficients require
• N2 complex multiplications
• N(N-1) complex additions
• Complexity in terms of real operations
• 4N2 real multiplications
• 2N(N-1) real additions
• Most fast methods are based on symmetry properties
– Conjugate symmetry
– Periodicity in n and k
1N
0k
knN/2jekXN1
]n[x
1N
0n
knN/2je]n[xkX
knNjnkNjkNNjnNkNj eeee /2/2/2/2
nNkNjNnkNjknNj eee /2/2/2
![Page 100: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/100.jpg)
Properties-Example
![Page 101: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/101.jpg)
Decimation-In-Time FFT Algorithms
• Makes use of both symmetry and periodicity• Consider special case of N an integer power of 2• Separate x[n] into two sequence of length N/2
– Even indexed samples in the first sequence– Odd indexed samples in the other sequence
• Substitute variables n=2r for n even and n=2r+1 for odd
• G[k] and H[k] are the N/2-point DFT’s of each subsequence
1
oddn
/21
evenn
/21
0
/2 ][][][N
knNjN
knNjN
n
knNj enxenxenxkX
kHWkG
WrxWWrx
WrxWrxkX
kN
Nrk
Nk
N
Nrk
N
Nkr
N
Nrk
N
]12[]2[
]12[]2[
12/
0r2/
12/
0r2/
12/
0r
1212/
0r
2
![Page 102: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/102.jpg)
Decimation In Time• 8-point DFT example using
decimation-in-time
• Two N/2-point DFTs
– 2(N/2)2 complex multiplications
– 2(N/2)2 complex additions
• Combining the DFT outputs
– N complex multiplications
– N complex additions
• Total complexity
– N2/2+N complex multiplications
– N2/2+N complex additions
– More efficient than direct DFT
• Repeat same process
– Divide N/2-point DFTs into
– Two N/4-point DFTs
– Combine outputs
![Page 103: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/103.jpg)
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DIT-FFT
![Page 105: UNIT-I DISCRETE FOURIER TRANSFORM. Syllabus Discrete Signals and Systems- A Review Introduction to DFT Properties of DFT Circular Convolution Filtering.](https://reader033.fdocuments.in/reader033/viewer/2022061607/56649e625503460f94b5d883/html5/thumbnails/105.jpg)
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Decimation In Time Cont’d
• After two steps of decimation in time
• Repeat until we’re left with two-point DFT’s
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Decimation-In-Time FFT Algorithm
• Final flow graph for 8-point decimation in time
• Complexity:
– Nlog2N complex multiplications and additions
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Butterfly Computation
• Flow graph constitutes of butterflies
• We can implement each butterfly with one multiplication
• Final complexity for decimation-in-time FFT– (N/2)log2N complex multiplications and additions
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In-Place Computation
• Decimation-in-time flow graphs require two sets of registers– Input and output for each stage
• Note the arrangement of the input indices– Bit reversed indexing
111x111X7x7X
011x110X3x6X
101x101X5x5X
001x100X1x4X
110x011X6x3X
010x010X2x2X
100x001X4x1X
000x000X0x0X
00
00
00
00
00
00
00
00
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Example: 8 point FFT
(1)Number of stages:
– Nstages = 3
(2)Blocks/stage:
– Stage 1: Nblocks = 4
– Stage 2: Nblocks = 2
– Stage 3: Nblocks = 1
(3)B’flies/block:
– Stage 1: Nbtf = 1
– Stage 2: Nbtf = 2
– Stage 3: Nbtf = 2
FFT Implementation
WW00-1-1
WW00-1-1
WW00-1-1
WW00-1-1
WW22-1-1
WW00
-1-1WW00
WW22-1-1
-1-1WW00
WW11-1-1
WW00
WW33-1-1
-1-1WW22
-1-1
Stage 2Stage 2 Stage 3Stage 3Stage 1Stage 1
• Decimation in time FFT:– Number of stages = log2N
– Number of blocks/stage = N/2stage
– Number of butterflies/block = 2stage-1
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FFT Implementation
Start IndexStart Index 00
Input IndexInput Index 11
Twiddle Factor IndexTwiddle Factor Index N/2 = 4N/2 = 4 44/2 = 2/2 = 2 22/2 = 1/2 = 1
Indicies UsedIndicies Used WW00 WW00
WW22
WW00
WW11
WW22
WW33
0022
0044
WW00-1-1
WW00-1-1
WW00-1-1
WW00-1-1
WW22-1-1
WW00
-1-1WW00
WW22-1-1
-1-1WW00
WW11-1-1
WW00
WW33-1-1
-1-1WW22
-1-1
Stage 2Stage 2 Stage 3Stage 3Stage 1Stage 1
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Decimation-in-time FFT algorithm
Most conveniently illustrated by considering the special case of N an integer power of 2, i.e, N=2v.
Since N is an even integer, we can consider computing X[k] by separating x[n] into two (N/2)-point sequence consisting of the even numbered point in x[n] and the odd-numbered points in x[n].
or, with the substitution of variable n=2r for n even and n=2r+1 for n odd
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Since
That is, WN2 is the root of the equation WN/2=1
Consequently,
Both G[k] and H[k] can be computed by (N/2)-point DFT, where G[k] is the (N/2)-point DFT of the even numbered points of the original sequence and the second being the (N/2)-point DFT of the odd-numbered point of the original sequence.Although the index ranges over N values, k = 0, 1, …, N-1, each of the sums must be computed only for k between 0 and (N/2)-1, since G[k] and H[k] are each periodic in k with period N/2.
2/)2//(2)/2(22
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Decomposing N-point DFT into two (N/2)-point DFT for the case of N=8
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We can further decompose the (N/2)-point DFT into two (N/4)-point DFTs. For example, the upper half of the previous diagram can be decomposed as
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Hence, the 8-point DFT can be obtained by the following diagram with four 2-point DFTs.
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Flow graph of a 2-point DFT
Finally, each 2-point DFT can be implemented by the following signal-flow graph, where no multiplications are needed.
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Flow graph of complete decimation-in-time decomposition of an 8-point DFT.
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In each stage of the decimation-in-time FFT algorithm, there are a basic structure called the butterfly computation:
The butterfly computation can be simplified as follows:
Flow graph of a basic butterfly computation in FFT.
Simplified butterfly computation.
][][][
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Flow graph of 8-point FFT using the simplified butterfly computation
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In the above, we have introduced the decimation-in-time algorithm of FFT.
Here, we assume that N is the power of 2. For N=2v, it requires v=log2N stages of computation.
The number of complex multiplications and additions required was N+N+…N = Nv = N log2N.
When N is not the power of 2, we can apply the same principle that were applied in the power-of-2 case when N is a composite integer. For example, if N=RQ, it is possible to express an N-point DFT as either the sum of R Q-point DFTs or as the sum of Q R-point DFTs.
In practice, by zero-padding a sequence into an N-point sequence with N=2v, we can choose the nearest power-of-two FFT algorithm for implementing a DFT.
The FFT algorithm of power-of-two is also called the Cooley-Tukey algorithm since it was first proposed by them.
For short-length sequence, Goertzel algorithm might be more efficient.
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Decimation-In-Frequency FFT Algorithm• Final flow graph for 8-point decimation in
frequency
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Decimation-In-Frequency FFT Algorithm
• The DFT equation
• Split the DFT equation into even and odd frequency indexes
• Substitute variables to get
• Similarly for odd-numbered frequencies
1N
0n
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Decimation in Frequency algorithm
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Decimation in Frequency
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DIF-FFT ALGORITHM
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DIF-FFT ALGORITHM
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Example
• Using decimation-in-time FFT algorithm compute DFT of the sequence
{-1 –1 –1 –1 1 1 1 1}• Solution: Twiddle factors are
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Solution and signal flow graph of the example
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IDFT Using DIF-FFT
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