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Chapter 11 Filters and Tuned Amplifiers Passive LC Filters Inductorless Filters Active-RC Filters Switched Capacitors

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Chapter 11 Filters and Tuned Amplifiers Passive LC Filters Inductorless Filters Active-RC Filters Switched Capacitors - PowerPoint PPT Presentation


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Chapter 11 Filters and Tuned Amplifiers Passive LC Filters Inductorless Filters Active-RC Filters Switched Capacitors. Filter Transmission, Types and Specification. Linear Filters. Filter Specification.

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Presentation Transcript
slide1

Chapter 11

  • Filters and Tuned Amplifiers
    • Passive LC Filters
    • Inductorless Filters
    • Active-RC Filters
    • Switched Capacitors
slide3

Filter Specification

Specification of the transmission characteristics of a low-pass filter. The magnitude response of a filter that just meets specifications is also shown.

  • Frequency-Selection function
    • Passing
    • Stopping
    • Pass-Band
    • Low-Pass
    • High-Pass
    • Band-Pass
    • Band-Stop
    • Band-Reject

Summary – Low-pass specs

-the passband edge

-the maximum allowed variation in passband, Amax

-the stopband edge

-the minimum required stopband attenuation, Amin

Passband ripple

Ripple bandwidth

slide4

Filter Specification

Transmission specifications for a bandpass filter. The magnitude response of a filter that just meets specifications is also shown. Note that this particular filter has a monotonically decreasing transmission in the passband on both sides of the peak frequency.

slide6

The Filter Transfer Function

Pole-zero pattern for the low-pass filter whose transmission is shown.

This filter is of the fifth order (N = 5.)

slide7

The Filter Transfer Function

Pole-zero pattern for the bandpass filter whose transmission is shown. This filter is of the sixth order (N = 6.)

slide8

Butterworth Filters

The magnitude response of a Butterworth filter.

slide9

Butterworth Filters

Magnitude response for Butterworth filters of various order with  = 1. Note that as the order increases, the response approaches the ideal brickwall type transmission.

slide10

Butterworth Filters

Graphical construction for determining the poles of a Butterworth filter of order N. All the poles lie in the left half of the s-plane on a circle of radius 0 = p(1/)1/N, where  is the passband deviation parameter :

(a) the general case, (b)N = 2, (c)N = 3, (d)N = 4.

slide11

Chebyshev Filters

Sketches of the transmission characteristics of a representative even- and odd-order Chebyshev filters.

slide14

First-Order Filter Functions

Fig. 11.14 First-order all-pass filter.

slide18

The Second-order LCR Resonator

Realization of various second-order filter functions using the LCR resonator of Fig.11.17(b): (a) general structure, (b) LP, (c) HP, (d) BP, (e) notch at 0, (f) general notch, (g) LPN (n0), (h) LPN as s , (i) HPN (n < 0).

slide19

The Second-Order Active Filter – Inductor Replacement

The Antoniou inductance-simulation circuit. (b) Analysis of the circuit assuming ideal op amps. The order of the analysis steps is indicated by the circled numbers.

slide20

The Second-Order Active Filter – Inductor Replacement

Realizations for the various second-order filter functions using the op amp-RC resonator of Fig.11.21(b). (a) LP; (b) HP; (c) BP, (d) notch at 0;

slide21

The Second-Order Active Filter – Inductor Replacement

(e) LPN, n0; (f) HPN, n0; (g) all-pass. The circuits are based on the LCR circuits in Fig.11.18. Design equations are given in Table11.1.

slide26

The Second-Order Active Filter – Two-Integrator-Loop

Derivation of an alternative two-integrator-loop biquad in which all op amps are used in a single-ended fashion. The resulting circuit in (b) is known as the Tow-Thomas biquad.

slide27

Fig. 11.26 The Tow-Thomas biquad with feedforward. The transfer function of Eq. (11.68) is realized by feeding the input signal through appropriate components to the inputs of the three op amps. This circuit can realize all special second-order functions. The design equations are given in Table 11.2.

slide29

Fig. 11.47 Obtaining a second-order narrow-band bandpass filter by transforming a first-order low-pass filter. (a) Pole of the first-order filter in the p-plane. (b) Applying the transformation s = p + j0 and adding a complex conjugate pole results in the poles of the second-order bandpass filter. (c) Magnitude response of the firs-order low-pass filter. (d) Magnitude response of the second-order bandpass filter.

slide30

Fig. 11.48 Obtaining the poles and the frequency response of a fourth-order stagger-tuned narrow-band bandpass amplifier by transforming a second-order low-pass maximally flat response.