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Chapter 17. Frequency Characteristics of AC Circuits. Introduction A High-Pass RC Network A Low-Pass RC Network A Low-Pass RL Network A High-Pass RL Network A Comparison of RC and RL Networks Bode Diagrams Combining the Effects of Several Stages RLC Circuits and Resonance

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Frequency Characteristics of AC Circuits


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frequency characteristics of ac circuits

Chapter 17

Frequency Characteristics of AC Circuits
  • Introduction
  • A High-Pass RC Network
  • A Low-Pass RC Network
  • A Low-Pass RL Network
  • A High-Pass RL Network
  • A Comparison of RC and RL Networks
  • Bode Diagrams
  • Combining the Effects of Several Stages
  • RLC Circuits and Resonance
  • Filters
  • Stray Capacitance and Inductance
introduction

17.1

Introduction
  • Earlier we looked at the bandwidth and frequency response of amplifiers
  • Having now looked at the AC behaviour of components we can consider these in more detail
  • The reactance of both inductors and capacitance is frequency dependent and we know that
slide3
We will start by considering very simple circuits
  • Consider the potential divider shown here
  • from our earlier consideration of the circuit
  • rearranging, the gain of the circuit is
  • this is also called the transfer function of the circuit
a high pass rc network

17.2

A High-Pass RC Network
  • Consider the following circuit
    • which is shown re-drawn in a more usual form
slide5
Clearly the transfer function is
  • At high frequencies
    •  is large, voltage gain  1
  • At low frequencies
    •  is small, voltage gain  0
slide6
Since the denominator has real and imaginary parts, the magnitude of the voltage gain is
  • When 1/CR = 1
  • This is a halving of power, or a fall in gain of 3 dB
slide7
The half power point is the cut-off frequency of the circuit
    • the angular frequency C at which this occurs is given by
    • where  is the time constant of the CR network. Also
slide8
Substituting  =2f and CR = 1/ 2fC in the earlier equation gives
  • This is the general form of the gain of the circuit
  • It is clear that both the magnitude of the gain and the phase angle vary with frequency
slide9
Consider the behaviour of the circuit at different frequencies:
  • When f >> fc
    • fc/f << 1, the voltage gain  1
  • When f = fc
  • When f << fc
slide10
The behaviour in these three regions can be illustrated using phasor diagrams
  • At low frequencies the gain is linearly related to frequency. It falls at -6dB/octave (-20dB/decade)
slide11
Frequency response of the high-pass network
    • the gain response hastwo asymptotes thatmeet at the cut-offfrequency
    • figures of this form are called Bode diagrams
a low pass rc network

17.3

A Low-Pass RC Network
  • Transposing the C and R gives
  • At high frequencies
    •  is large, voltage gain  0
  • At low frequencies
    •  is small, voltage gain  1
a low pass rc network13

17.3

A Low-Pass RC Network
  • A similar analysis to before gives
  • Therefore when, when CR = 1
  • Which is the cut-off frequency
slide14
Therefore
    • the angular frequency C at which this occurs is given by
    • where  is the time constant of the CR network, and as before
slide15
Substituting  =2f and CR = 1/ 2fC in the earlier equation gives
  • This is similar, but not the same, as the transfer function for the high-pass network
slide16
Consider the behaviour of this circuit at different frequencies:
  • When f << fc
    • f/fc<< 1, the voltage gain  1
  • When f = fc
  • When f >> fc
slide17
The behaviour in these three regions can again be illustrated using phasor diagrams
  • At high frequencies the gain is linearly related to frequency. It falls at 6dB/octave (20dB/decade)
slide18
Frequency response of the low-pass network
    • the gain response hastwo asymptotes thatmeet at the cut-offfrequency
    • you might like to compare this with the Bode Diagram for a high-pass network
a low pass rl network

17.4

A Low-Pass RL Network
  • Low-pass networks can alsobe produced using RL circuits
    • these behave similarly to thecorresponding CR circuit
    • the voltage gain is
    • the cut-off frequency is
a high pass rl network

17.5

A High-Pass RL Network
  • High-pass networks can alsobe produced using RL circuits
    • these behave similarly to thecorresponding CR circuit
    • the voltage gain is
    • the cut-off frequency is
a comparison of rc and rl networks

17.6

A Comparison of RC and RL Networks
  • Circuits using RC and RLtechniques have similarcharacteristics
    • for a more detailedcomparison, seeFigure 17.10 in thecourse text
bode diagrams

17.7

Bode Diagrams
  • Straight-line approximations
combining the effects of several stages

17.8

Combining the Effects of Several Stages
  • The effects of several stages ‘add’ in bode diagrams
slide25
Multiple high- and low-passelements may also be combined
    • this is illustrated in Figure 17.14in the course text
rlc circuits and resonance

17.9

RLC Circuits and Resonance
  • Series RLC circuits
    • the impedance is given by
    • if the magnitude of the reactanceof the inductor and capacitor areequal, the imaginary part is zero,and the impedance is simply R
    • this occurs when
slide27
This situation is referred to as resonance
    • the frequency at which is occurs is the resonant frequency
    • in the series resonant circuit, the impedance is at a minimum at resonance
    • the current is at a maximum at resonance
slide28
The resonant effect can be quantified by the quality factor, Q
    • this is the ratio of the energy dissipated to the energy stored in each cycle
    • it can be shown that
    • and
slide29
The series RLC circuit is an acceptor circuit
    • the narrowness of bandwidth is determined by the Q
    • combining this equation with the earlier one gives
slide31
The parallel arrangement is a rejector circuit
    • in the parallel resonant circuit, the impedance is at a maximum at resonance
    • the current is at a minimum at resonance
    • in this circuit
filters

17.10

Filters
  • RC Filters
  • The RC networks considered earlier are first-order or single-pole filters
    • these have a maximum roll-off of 6 dB/octave
    • they also produce a maximum of 90 phase shift
  • Combining multiple stages can produce filters with a greater ultimate roll-off rates (12 dB, 18 dB, etc.) but such filters have a very soft ‘knee’
slide33
An ideal filter would have constant gain and zero phase shift for frequencies within its pass band, and zero gain for frequencies outside this range (its stop band)
  • Real filters do not have theseidealised characteristics
slide34
LC Filters
  • Simple LC filters can be produced using series or parallel tuned circuits
    • these produce narrow-band filters with a centre frequency fo
slide35
Active filters
    • combining an op-amp with suitable resistors and capacitors can produce a range of filter characteristics
    • these are termed active filters
slide36
Common forms include:
  • Butterworth
    • optimised for a flat response
  • Chebyshev
    • optimised for a sharp ‘knee’
  • Bessel
    • optimised for its phase response

see Section 17.10.3 of the course text for more information on these

stray capacitance and inductance

17.11

Stray Capacitance and Inductance
  • All circuits have stray capacitance and stray inductance
    • these unintended elements can dramatically affect circuit operation
    • for example:
      • (a) Cs adds an unintended low-pass filter
      • (b) Ls adds an unintended low-pass filter
      • (c) Cs produces an unintended resonant circuit and can produce instability
key points
Key Points
  • The reactance of capacitors and inductors is dependent on frequency
  • Single RC or RL networks can produce an arrangement with a single upper or lower cut-off frequency.
  • In each case the angular cut-off frequency o is given by the reciprocal of the time constant
  • For an RC circuit  = CR, for an RL circuit  = L/R
  • Resonance occurs when the reactance of the capacitive element cancels that of the inductive element
  • Simple RC or RL networks represent single-pole filters
  • Active filters produce high performance without inductors
  • Stray capacitance and inductance are found in all circuits