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Chapter 7 Finite Impulse Response(FIR) Filter Design
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1. Features of FIR filter Characteristic of FIR filter
FIR filter is always stable FIR filter can have an exactly linear phase response FIR filter are very simple to implement. Nonrecursive FIR filters suffer less from the effect of finite wordlength than IIR filters
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2. Linear phase response Phase response of FIR filter
Phase delay and group delay (1) where (2)
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Condition of linear phase response
(3) (4) Where and is constant Constant group delay and phase delay response
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If a filter satisfies the condition given in equation (3)
From equation (1) and (2) thus
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It is represented in Fig 7.1 (a),(b)
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When the condition given in equation (4) only
The filter will have a constant group delay only It is represented in Fig 7.1 (c),(d)
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Center of symmetry Fig. 7-1.
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Table 7.1 A summary of the key point about the four types of linear phase FIR filters
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Example 7-1 Symmetric impulse response for linear phase response. No phase distortion
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Frequency response where
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(3) where
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3. Zero distribution of FIR filters
Transfer function for FIR filter
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Four types of linear phase FIR filters
have zero at is real and is imaginary
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If zero on unit circle If zero not exist on the unit circle If zeros on
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Necessary zero Necessary zero Necessary zero Necessary zero Fig. 7-2.
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4. FIR filter specifications
peak passband deviation (or ripples) stopband deviation passband edge frequency stopband edge frequency sampling frequency
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ILPF Satisfies spec’s Fig. 7-3.
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Characterization of FIR filter
Most commonly methods for obtaining Window, optimal and frequency sampling methods
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5. Window method FIR filter Frequency response of filter
Corresponding impulse response Ideal lowpass response
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Fig. 7-4.
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Truncation to FIR Rectangular Window
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Fig. 7-5.
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Fig. 7-6.
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Fig. 7-7.
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Table 7.2 summary of ideal impulse responses for standard frequency selective filters
and are the normalized passband or stopband edge frequencies; N is the length of filter
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Common window function types
Hamming window where N is filter length and is normalized transition width
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Characteristics of common window functions
Fig. 7-8.
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Table 7.3 summary of important features of common window functions
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Kaiser window where is the zero-order modified Bessel function of the first kind where typically
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Kaiser Formulas – for LPF design
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Example 7-2 Obtain coefficients of FIR lowpass using hamming window
Lowpass filter Passband cutoff frequency Transition width Stopband attenuation Sampling frequency
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Using Hamming window
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Fig. 7-9.
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Example 7-3 Obtain coefficients using Kaiser or Blackman window
Stopband attenuation passband attenuation Transition region Sampling frequency Passband cutoff frequency
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Using Kaiser window
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Fig
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Summary of window method
1. Specify the ‘ideal’ or desired frequency response of filter, 2. Obtain the impulse response, , of the desired filter by evaluating the inverse Fourier transform 3. Select a window function that satisfies the passband or attenuation specifications and then determine the number of filter coefficients 4. Obtain values of for the chosen window function and the values of the actual FIR coefficients, , by multiplying by
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Advantages and disadvantages
Simplicity Lack of flexibility The passband and stopband edge frequencies cannot be precisely specified For a given window(except the Kaiser), the maximum ripple amplitude in filter response is fixed regardless of how large we make N
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6. The optimal method Basic concepts Equiripple passband and stopband
For linear phase lowpass filters m+1 or m+2 extrema(minima and maxima) Weighted Approx. error Weighting function Ideal desired response Practical response where m=(N+1)/2 (for type1 filters) or m =N/2 (for type2 filters)
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Practical response Ideal response Fig
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Fig
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Optimal method involves the following steps
Use the Remez exchange algorithm to find the optimum set of extremal frequencies Determine the frequency response using the extremal frequencies Obtain the impulse response coefficients
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Optimal FIR filer design
where where and , Let This weighting function permits different peak error in the two band
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where are and Find
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Alternation theorem Let
If has equiripple inside bands and more than m+2 extremal point then where
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From equation (7-33) and (7-34)
Equation (7-35) is substituted equation (7-32) Matrix form
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Summary Step 1. Select filter length as 2m+1
Step 2. Select m point in F Step 3. Calculate and e using equation (7) Step 4. Calculate using equation (5). If in some of f , go to step 5, otherwise go to step 6 Step 5. Determine m local minma or maxma points Step 6. Calculate when where
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Example 7-4 Specification of desired filter Ideal low pass filter
Filter length : 3 Normalized frequency
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From Cutoff frequency : not the optimal filter
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: has the minimum (N=3)
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Fig
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Optimization using MATLAB
Park-McClellan Remez where N is the filter order (N+1 is the filter length) F is the normalized frequency of border of pass band M is the magnitude of frequency response WT is the weight between ripples
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Example 7-5 Specification of desired filter
Band pass region : 0 – 1000Hz Transition region : 500Hz Filter length : 45 Sampling frequency : 10,000Hz Normalized frequency of border of passband Magnitude of frequency response
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Table 7-4.
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Fig.7-14.
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Example 7-6 Specification of desired filter
Band pass region : 3kHz – 4kHz Transition region : 500Hz Pass band ripple : 1dB Rejection region : 25dB Sampling frequency : 20kHz Frequency of border of passband
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Transform dB to normal value
Filter length Remezord (MATLAB command) where and ripple value(dB) of pass band and rejection band
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Table 7-5.
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Fig
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7. Frequency sampling method
Frequency sampling filters Taking N samples of the frequency response at intervals of Filter coefficients where are samples of the ideal or target frequency response
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For linear phase filters (for N even)
For N odd Upper limit in summation is where
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Fig
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Example 7-7 (1) Show the Expanding the equation is real value
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Sampling frequency : 18kHz Filter length : 9
(2) Design of FIR filter Band pass region : 0 – 5kHz Sampling frequency : 18kHz Filter length : 9 Fig
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Samples of magnitude in frequency
Table 7-6.
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8. Comparison of most commonly method
Window method The easiest, but lacks flexibility especially when passband and stopband ripples are different Frequency sampling method Well suited to recursive implementation of FIR filters Optimal method Most powerful and flexible
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