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WINDOWING TECHNIQUES OF
FIR FILTER DESIGN
Presented by,
SoumilAgarwal (J001), Aayush Maheshwari (J015), Rohan Nagpal (J019),Vibhuti Maheshwari (J036)
WHAT IS AWINDOWING?
A window is a finite length sequence.
Windowing is a process of forming a finite length
sequence from an infinite length sequence by
multiplying an infinite length sequence with a window.
GENERAL PROCEDURE FORWINDOWING
1. Choose the desired frequency response of the filter Hd (ω)
2. Take inverse fourier transform of Hd (ω) to obtain the desired impulse response hd
(n)
3. Choose a window sequence W(n) and multiply hd (n) by Hd (n) to convert IIR to FIR
h(n)=W(n) x hd (n)
4. Taking ZT of h(n) we obtain a transfer function H(z)
5. Realize the filter using suitable filter method
TYPES OF WINDOWS
WINDOWS
Rectangular Hanning Hamming Blackman Bartlett
Depending on the stop band attenuation we will select a window. Stop band attenuation (As) are the
lower limits of attenuation.
For example, if As is 40 dB, we will choose HanningWindow
WINDOW EQUATIONS
EXAMPLE
STEP 1- CHOOSETHE DESIRED FREQUENCY
STEP 2 –TO FIND Hd (n)
STEP 3 – CONVERSION OF FINITETO
INFINITE SERIES
STEP 4–TO FIND H(z)
STEP 5 - LINEAR PHASE REALISATION
ADVANTAGES AND DISADVANTAGES
 Simple – involves minimum computation
 Maximum ripple amplitude in filter response is fixed regardless of how large the
filter order is
 Lack of flexibility
 When the expression for the desired filter response Hd(e^jw) is complicated or
cannot be put into a closed form mathematical expression, evaluation of Hd(n)
becomes difficult.
THANKYOU

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Windowing techniques of fir filter design

  • 1. WINDOWING TECHNIQUES OF FIR FILTER DESIGN Presented by, SoumilAgarwal (J001), Aayush Maheshwari (J015), Rohan Nagpal (J019),Vibhuti Maheshwari (J036)
  • 2. WHAT IS AWINDOWING? A window is a finite length sequence. Windowing is a process of forming a finite length sequence from an infinite length sequence by multiplying an infinite length sequence with a window.
  • 3. GENERAL PROCEDURE FORWINDOWING 1. Choose the desired frequency response of the filter Hd (ω) 2. Take inverse fourier transform of Hd (ω) to obtain the desired impulse response hd (n) 3. Choose a window sequence W(n) and multiply hd (n) by Hd (n) to convert IIR to FIR h(n)=W(n) x hd (n) 4. Taking ZT of h(n) we obtain a transfer function H(z) 5. Realize the filter using suitable filter method
  • 4. TYPES OF WINDOWS WINDOWS Rectangular Hanning Hamming Blackman Bartlett Depending on the stop band attenuation we will select a window. Stop band attenuation (As) are the lower limits of attenuation. For example, if As is 40 dB, we will choose HanningWindow
  • 7. STEP 1- CHOOSETHE DESIRED FREQUENCY
  • 8. STEP 2 –TO FIND Hd (n)
  • 9. STEP 3 – CONVERSION OF FINITETO INFINITE SERIES
  • 11. STEP 5 - LINEAR PHASE REALISATION
  • 12. ADVANTAGES AND DISADVANTAGES  Simple – involves minimum computation  Maximum ripple amplitude in filter response is fixed regardless of how large the filter order is  Lack of flexibility  When the expression for the desired filter response Hd(e^jw) is complicated or cannot be put into a closed form mathematical expression, evaluation of Hd(n) becomes difficult.