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Active Filters

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Active Filters Conventional passive filters consist of LCR networks. Inductors are undesirable components: They are particularly non-ideal (lossy) – PowerPoint PPT presentation

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Title: Active Filters


1
Active Filters
  • Conventional passive filters consist of LCR
    networks.
  • Inductors are undesirable components
  • They are particularly non-ideal (lossy)
  • They are bulky and expensive
  • Active filters replace inductors using op-amp
    based equivalent circuits.

2
Active Filter Designs
  • Three active filter design techniques will be
    covered
  • Synthesis by Sections
  • Cascade of second order sections.
  • Component Simulation
  • Replace inductors with op-amp inductor
    simulations.
  • Operational Simulation
  • Simulate all currents and voltages in the LCR
    ladder using an analogue computer.

3
Analogue Filter Responses
H(f)
H(f)
0
0
f
f
fc
fc
Ideal brick wall filter
Practical filter
4
Standard Transfer Functions
  • Butterworth
  • Flat Pass-band.
  • 20n dB per decade roll-off.
  • Chebyshev
  • Pass-band ripple.
  • Sharper cut-off than Butterworth.
  • Elliptic
  • Pass-band and stop-band ripple.
  • Even sharper cut-off.
  • Bessel
  • Linear phase response i.e. no signal distortion
    in pass-band.

5
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6
Analogue Transfer Functions
The transfer function of any analogue filter
(active or passive) can be expressed as the ratio
of two polynomials
7
Poles and Zeros
  • Poles
  • Complex values of s where the transfer function
    is infinite.
  • i.e. the denominator of the transfer function is
    zero.
  • Zeros
  • Complex values of s where the transfer function
    is zero.
  • An N-th order filter will have N poles and up to
    N zeros.
  • Some poles may be in the same place (as may some
    zeros).

8
Example Two Pole Bessel Filter
Low pass, cut-off frequency 1 rad/s, from
tables
9
Operational Amplifiers
  • All the active filters we shall study are based
    on operational amplifiers (op-amps).
  • Analysis of linear op-amp circuits is usually
    based on simplifying assumptions
  • The difference between the non-inverting and
    inverting inputs is zero.
  • The input current is zero.
  • The output voltage and current is arbitrary.

10
Op-Amp Assumptions
I
V

Iout
Vout
I-
-
V-
11
Inverting Amplifier
Z2
Z1
VIN
-
VOUT

0 V
12
Non-Inverting Amplifier

VIN
VOUT
-
Z1
Z2
0 V
13
Buffer Amplifier

VIN
VOUT
-
  • Output voltage Input voltage
  • Input impedance is infinite
  • Output impedance is zero

14
Single-Pole Passive Filter
R
C
vin
vout
  • First order low pass filter
  • Cut-off frequency 1/CR rad/s
  • Problem Any load (or source) impedance will
    change frequency response.

15
Single-Pole Active Filter
R
C
vin
vout
  • Same frequency response as passive filter.
  • Buffer amplifier does not load RC network.
  • Output impedance is now zero.

16
Low-Pass and High-Pass Designs
High Pass
Low Pass
17
Higher Order Filters
  • You might think we could make higher order
    filters by simply cascading N first order filters
  • This doesnt work
  • The single pole of a first order filter must be
    purely real (no imaginary part)
  • The poles of a higher order filter usually need
    to be complex
  • Solution Use second order sections, each one
    synthesising a conjugate pair of complex poles

18
Summary
  • Active filter designs aim to replace the
    inductors in passive filters.
  • Design techniques
  • Synthesis by sections
  • Component simulation
  • Operational simulation
  • All based on op-amps understanding of basic
    op-amp circuits is essential.
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