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VFO FIR differintegrator, pure differentiator and pure integrator examples

在文檔中 可調式數位濾波器之設計 (頁 43-0)

Chapter 5. Design of Variable Fractional-Order FIR Differintegrators

5.3 VFO FIR differintegrator, pure differentiator and pure integrator examples

The design example 1 deals with a VFO FIR differintegrator with N =40, M =5, ωs =0.05π,

f 0.95

ω = π , ps= −0.5, pf =0.5 and W

( )

ω =1. Figs. 5-2(a) and (b) display the variable magnitude response and the absolute error of variable frequency response, respectively. For example 2, a pure VFO differentiator is designed with N =30, M =6, ωs =0, ωf =0.9π, , and . The variable magnitude response and the absolute error of variable frequency response are shown in Figs. 5-3(a) and (b). Then, consider the design of a VFO integrator

with , ,

Similarly, Fig. 5-4(a) presents the variable magnitude response and Fig. 5-4(b) displays the absolute error of variable frequency response. Notice that, this technique can also be applied when is odd.

N

(a)

(b)

Fig. 5-2 Design of a VFO differintegrator with

f 0.95

ω = π, ps = −0.5, and pf =0.5 (a) Variable magnitude response (b) Absolute error of variable frequency response.

, , M =5 , ωs =0.05π 40

N =

(b)

Fig. 5-3 Design of a VFO differentiator with N =30, M =6, ωs =0, ωf =0.9π, 1ps = , (a)

and 2pf = (a) Variable magnitude response (b) Absolute e y respo

rror of variable frequenc nse.

(a)

(b)

Fig. 5-4 Design of a VFO integrator with N =60, M =6 , ωs =0.05π , ωf =0.9π ,

s 1.5

p = − , and pf = −0.5 (a) Variable magnitude resp nse (b) bsolute erro of variableo A r frequency response.

5.4 Conclusions

In this section, the design of the variable fractional-order FIR differintegrators is summarized. The technique of Weighted Least-Squares Approach was proposed for designing the VFO FIR differintegrators. Besides, the symmetric and antisymmetric characteristics were also applied to the coefficients of the VFO FIR filters. As a result, not only even N but also odd N can be used by this method. Finally, some design examples, including a VFO FIR differintegrator, a pure VFO differentiators and a pure VFO integrator, were presented to demonstrate the design effectiveness.

Chapter 6

Design of Variable Fractional-Order IIR Differintegrators

6.1 Introduction

In this chapter, the design of the VFO IIR differintegrators based on IIR-typed Farrow structure is pr

zed as follows: problem formulation is derived step by step in section 6.2.

Se

6.2 Problem Formulation

For designing the VFO differintegrator, the desired response is given by

oposed. For designing the IIR digital filters, the issue of the stability is significant concerned [39]-[40]. By incorporating a constrained function into the objective error function, the stability of the VFO IIR digital filters can be overcome. To achieve the results which satisfy the stable condition and simplify the calculations, a quadratic method is successfully used to deal with this highly nonlinear problem [41].

This chapter is organi

ction 6.3 gives three examples, containing a VFO IIR differintegrator, a pure VFO IIR differentiator, and a pure VFO IIR integrator. At last, the conclusions are summarized in section 6.4.

(

,

) ( )

ˆ

(

,

)

ω > , it is a VFO differintegrator. The subscripts s and f denotes the start points and final of the adjustable region and the designed band.

Let

where means a sign function.

oxima e used transfer function of VFO IIR filter is

( )

sgn .

To appr te the desired response, th

( ) ( )

ubstituting (6.4a) and (6.4b) into (6.3) can yield

( ) ( )

( ) ( )

otice that, (6.5) can be implemented by IIR-typed Farrow structure as shown in Fig. 6-1.

( ) ( )

Fig. 6-1 IIR-typed Farrow structure

As a result, the frequency response of the desired filter can be formulated into

( ) ( ( ) )

here the superscript T denotes a transpose operator, w

( )

1, 0 ,...,

(

a, 0 ,...,

) (

1,

)

,...,

(

a,

)

T (6.8 )

Thus, the approximation error function can be gotten by

( ) ( ) ( )

oncerning the stability of the VFO IIR digital filter, it has been shown in [41] that C

of

ust be small enough to satisfy the stable condition. The con rained function is def

( ) ( )

herefore, the objective error function of the VFO IIR digital filter can be given by T

li or function is expressed as

To simp fy the calculation, the objective err

(

,

)

,

(

,

)

,

( )

(6.15 ) Then, (6.13) becomes

( ) ( ) ( )

Additionally, the integrand of the constrained function can be formulated into

( )

2

Significantly, the constrained function would become

( )

So the original nonlinear problem in (6.12) can be converted into a quadratic problem, and the objective error function is indicated as

( )

,

( )

,

( )

Furthermore, by differentiating with respect to , and setting the result to zero, the solution can be obtained as below:

( )

k

6.3 VFO FIR differintegrator, pure differentiator and pure integrator examples

Three examples are designed in this section. For example 1, it deals with a VFO IIR differintegrator with I =19, Na =11, Nb =29 , M =5, ωs =0.05π , ωf =0.95π , 0.5ps = − and , and shows the results in Figs. 6-2(a) and (b), which are the magnitude response and absolute error of variable frequency response. A pure VFO IIR differentiator with

f 0.5 presents the magnitude response of a pure VFO IIR differentiator. Besides, Fig. 6-3(b) displays the absolute error of variable frequency response. Then, consider the design of a pure VFO IIR integrator with I =28, Na =15, Nb =45, 4M = , ωs =0.05π , ωf =0.9π , , and in the example 3. Similarly, the magnitude response and the absolute error of variable frequency response of a pure VFO IIR integrator are illustrated in Figs. 6-4(a) and (b).

s 1.5 p = −

= −0.5 pf

(a)

(b)

Fig. 6-2 Design of a Na =11, Nb =29, M =5, ωs =0.05π, ωf =0.95π, ,

, and

s 0.5 p = −

f 0.5

p = α =1.77827294×105 I =19 VFO IIR differintegrator. (a) Magnitude response (b) Absolute error of variable frequency response.

(a)

(b)

(b) Absolute error of variable frequency response.

Fig. 6-3 Design of a Na =7, Nb =23, M =3, ωs =0, ωf =0.9π , , ps =1 pf = , 2 and VFO IIR differentiator (a) Magnitude response 1.77827294 10 4

α = × I =14

(a)

(b)

Fig. 6-4 Design of a Na =15, Nb =45, 4M = , ωs =0.05π , ωf =0.9π , ,

, and

s 1.5 p = −

f 0.5

p = − α =5.62341325×102 I =28 VFO IIR integrator (a) Magnitude response (b) Absolute error of variable frequency response.

6.4 Conclusions

The design of the VFO IIR differintegrator, including the pure VFO IIR differentiator and the pure VFO IIR integrator, is summarized in this section. To implement it, IIR-typed Farrow structure was proposed. A quadratic method was used to overcome the highly nonlinear problem of the objective error function and simplify the calculations. However, the relative weighting constant α was different in all design examples because it must be properly chosen in order to ensure the stability of the designed filters. To show the performance, three examples were presented. In these three examples, the frequency ω and the variable parameter p were sampled similarly, which were and

(

, respectively. Finally, the results of this method are illustrated in Figs. 6-2, 6-3, and 6-4.

(

ωf ωs

)

/ 200 pf ps

)

/ 200

Chapter 7

Conclusions and Future works

In this thesis, it is focused on investigating the various designs of variable digital filters. These designs are all discussed in detail. First, the research topic is concentrated on the variable fractional-delay (VFD) filters. The VFD FIR, VFD IIR, and VFD Allpass filters are designed in chapters 2, 3, and 4. Weighted Least-Squares Approach (WLS) has been successfully used to achieve the desired results, including the magnitude response, the group-delay response, the absolute error of variable frequency response, and the absolute group-delay error. As for the IIR and Allpass filters, they are more difficult to realize than the FIR filters because their stability problem must be considerable attention. Fortunately, the desired VFD filter systems can be implemented by the Farrow structure.

Second, the variable fractional-order (VFO) differintegrators are also concerned. The VFO FIR differintegrators and the VFO IIR differintegrators are proposed to design in chapters 5 and 6, respectively. Besides, both the pure VFO differentiator and the pure VFO integrator can be realized by choosing the proper range of the parameter p . Similarly, the results can be obtained to demonstrate the performance as well. In addition, the VFO IIR differintegrators also must satisfy the stable condition. In the design procedure of this thesis, many techniques are applied to achieve the desired goals. Binomial Series Expansion and Taylor Series Expansion helpfully evaluate the related vectors or matrices in closed-forms. The symmetric or antisymmetric relationships of the filter coefficients are also widely used. When the highly nonlinear formulations occur, quadratic method can overcome them to simplify the calculations and complexity.

In the future, the research of the variable digital filters will be more developed due to their wide applications. Based on many past achievements in regard to this aspect, more and more methods and criteria will appear. So, this issue is still worthy of further study.

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