01100_freqresp

Upload: tejrajchitare

Post on 09-Oct-2015

8 views

Category:

Documents


0 download

DESCRIPTION

good

TRANSCRIPT

  • 5/19/2018 01100_Freqresp

    1/118

    11: Frequency Responses

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 1 / 12

  • 5/19/2018 01100_Freqresp

    2/118

    Frequency Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 2 / 12

    Ifx(t)is a sine wave, theny(t)will also be asine wave but with a different amplitude and

    phase shift.Xis an input phasor andY is theoutput phasor.

  • 5/19/2018 01100_Freqresp

    3/118

    Frequency Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 2 / 12

    Ifx(t)is a sine wave, theny(t)will also be asine wave but with a different amplitude and

    phase shift.Xis an input phasor andY is theoutput phasor.

    Thegainof the circuit is YX = 1/jCR+1/jC =

    1jRC+1

  • 5/19/2018 01100_Freqresp

    4/118

    Frequency Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 2 / 12

    Ifx(t)is a sine wave, theny(t)will also be asine wave but with a different amplitude and

    phase shift.Xis an input phasor andY is theoutput phasor.

    Thegainof the circuit is YX = 1/jCR+1/jC =

    1jRC+1

    This is a complex function of so we plot separate graphs for:

  • 5/19/2018 01100_Freqresp

    5/118

    Frequency Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 2 / 12

    Ifx(t)is a sine wave, theny(t)will also be asine wave but with a different amplitude and

    phase shift.Xis an input phasor andY is theoutput phasor.

    Thegainof the circuit is YX = 1/jCR+1/jC =

    1jRC+1

    This is a complex function of so we plot separate graphs for:

    Magnitude: YX=

    1|jRC+1| =

    1

    1+(RC)2

  • 5/19/2018 01100_Freqresp

    6/118

    Frequency Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 2 / 12

    Ifx(t)is a sine wave, theny(t)will also be asine wave but with a different amplitude and

    phase shift.Xis an input phasor andY is theoutput phasor.

    Thegainof the circuit is YX = 1/jCR+1/jC =

    1jRC+1

    This is a complex function of so we plot separate graphs for:

    Magnitude: YX=

    1|jRC+1| =

    1

    1+(RC)2

    0 1 2 3 4 50

    0.5

    1

    RC

    Magnitude Response

  • 5/19/2018 01100_Freqresp

    7/118

    Frequency Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 2 / 12

    Ifx(t)is a sine wave, theny(t)will also be asine wave but with a different amplitude and

    phase shift.Xis an input phasor andY is theoutput phasor.

    Thegainof the circuit is YX = 1/jCR+1/jC =

    1jRC+1

    This is a complex function of so we plot separate graphs for:

    Magnitude: YX=

    1|jRC+1| =

    1

    1+(RC)2Phase Shift:

    YX

    = (jRC+ 1) = arctan RC1

    0 1 2 3 4 50

    0.5

    1

    RC

    Magnitude Response

  • 5/19/2018 01100_Freqresp

    8/118

    Frequency Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 2 / 12

    Ifx(t)is a sine wave, theny(t)will also be asine wave but with a different amplitude and

    phase shift.Xis an input phasor andY is theoutput phasor.

    Thegainof the circuit is YX = 1/jCR+1/jC =

    1jRC+1

    This is a complex function of so we plot separate graphs for:

    Magnitude: YX=

    1|jRC+1| =

    1

    1+(RC)2Phase Shift:

    YX

    = (jRC+ 1) = arctan RC1

    0 1 2 3 4 50

    0.5

    1

    RC

    Magnitude Response

    0 1 2 3 4 5

    -0.4

    -0.2

    0

    RC

    Phase Response

  • 5/19/2018 01100_Freqresp

    9/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72

  • 5/19/2018 01100_Freqresp

    10/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase()

  • 5/19/2018 01100_Freqresp

    11/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    0 0.5 1

    -0.4

    -0.2

    0 X

    YX-Y

    =50

    Real

    Imag

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase()

  • 5/19/2018 01100_Freqresp

    12/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    0 0.5 1

    -0.4

    -0.2

    0 X

    YX-Y

    =50

    Real

    Imag

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72 0 20 40 60 80 100 120-1-0.5

    0

    0.5

    1

    x

    y

    time (ms)

    x=blue,y=red

    w = 50 rad/s, Gain = 0.89, Phase = -27

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase()

  • 5/19/2018 01100_Freqresp

    13/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase()

  • 5/19/2018 01100_Freqresp

    14/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    0 0.5 1

    -0.4

    -0.2

    0 X

    YX-Y

    =100

    Real

    Imag

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase()

  • 5/19/2018 01100_Freqresp

    15/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    0 0.5 1

    -0.4

    -0.2

    0 X

    YX-Y

    =100

    Real

    Imag

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72 0 20 40 60 80 100 120-1

    -0.5

    0

    0.5

    1

    x

    y

    time (ms)

    x=blue,y=red

    w = 100 rad/s, Gain = 0.71, Phase = -45

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase()

  • 5/19/2018 01100_Freqresp

    16/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase(

    )

  • 5/19/2018 01100_Freqresp

    17/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    0 0.5 1

    -0.4

    -0.2

    0 X

    YX-Y

    =300

    Real

    Imag

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase(

    )

  • 5/19/2018 01100_Freqresp

    18/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    0 0.5 1

    -0.4

    -0.2

    0 X

    YX-Y

    =300

    Real

    Imag

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72 0 20 40 60 80 100 120-1

    -0.5

    0

    0.5

    1

    x

    y

    time (ms)

    x=blue,y=red

    w = 300 rad/s, Gain = 0.32, Phase = -72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase(

    )

  • 5/19/2018 01100_Freqresp

    19/118

    Sine Wave Response

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 3 / 12

    RC= 10 ms

    YX =

    1jRC+1 =

    10.01j+1

    0 0.5 1

    -0.4

    -0.2

    0 X

    YX-Y

    =300

    Real

    Imag

    = 50 YX = 0.89 27

    = 100 YX = 0.71 45

    = 300 YX = 0.32 72 0 20 40 60 80 100 120-1

    -0.5

    0

    0.5

    1

    x

    y

    time (ms)

    x=blue,y=red

    w = 300 rad/s, Gain = 0.32, Phase = -72

    0 100 200 300 400 5000

    0.5

    1

    (rad/s)

    |Y/X|

    0 100 200 300 400 500

    -80

    -60

    -40

    -20

    0

    (rad/s)

    Phase(

    )

    The output,y(t),lagsthe input,x(t), by up to90.

  • 5/19/2018 01100_Freqresp

    20/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

  • 5/19/2018 01100_Freqresp

    21/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    0.1 1 10

    -0.4

    -0.2

    0

    RC

  • 5/19/2018 01100_Freqresp

    22/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    0.1 1 10-30

    -20

    -10

    0

    RC0.1 1 10

    -0.4

    -0.2

    0

    RC

  • 5/19/2018 01100_Freqresp

    23/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    Logarithmic voltage ratios are specified in decibels (dB)=20 log10|V2||V1| .

    0.1 1 10-30

    -20

    -10

    0

    RC0.1 1 10

    -0.4

    -0.2

    0

    RC

  • 5/19/2018 01100_Freqresp

    24/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    Logarithmic voltage ratios are specified in decibels (dB)=20 log10|V2||V1| .

    Common ratios:1 0 dB,

    0.1 1 10-30

    -20

    -10

    0

    RC0.1 1 10

    -0.4

    -0.2

    0

    RC

  • 5/19/2018 01100_Freqresp

    25/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    Logarithmic voltage ratios are specified in decibels (dB)=20 log10|V2||V1| .

    Common ratios:1 0 dB,10 20 dB, 0.1 20 dB, 100 40 dB,

    0.1 1 10-30

    -20

    -10

    0

    RC0.1 1 10

    -0.4

    -0.2

    0

    RC

  • 5/19/2018 01100_Freqresp

    26/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    Logarithmic voltage ratios are specified in decibels (dB)=20 log10|V2||V1| .

    Common ratios:1 0 dB,10 20 dB, 0.1 20 dB, 100 40 dB,2 6 dB, 0.5 6 dB,

    0.1 1 10-30

    -20

    -10

    0

    RC0.1 1 10

    -0.4

    -0.2

    0

    RC

  • 5/19/2018 01100_Freqresp

    27/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    Logarithmic voltage ratios are specified in decibels (dB)=20 log10|V2||V1| .

    Common ratios:1 0 dB,10 20 dB, 0.1 20 dB, 100 40 dB,2 6 dB, 0.5 6 dB,

    2 = 1.41 3 dB, 12

    = 0.707 3 dB.

    0.1 1 10-30

    -20

    -10

    0

    RC0.1 1 10

    -0.4

    -0.2

    0

    RC

  • 5/19/2018 01100_Freqresp

    28/118

    Logarathmic axes

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 4 / 12

    We usually use logarithmic axes for frequency and gain (but not phase)

    because % differences are more significant than absolute differences.

    E.g.5 kHz versus5.005 kHz is less significant than10 Hz versus15 Hzeven though both differences equal5 Hz.

    Logarithmic voltage ratios are specified in decibels (dB)=20 log10|V2||V1| .

    Common ratios:1 0 dB,10 20 dB, 0.1 20 dB, 100 40 dB,2 6 dB, 0.5 6 dB,

    2 = 1.41 3 dB, 12

    = 0.707 3 dB.

    0.1 1 10-30

    -20

    -10

    0

    RC0.1 1 10

    -0.4

    -0.2

    0

    RC

    Note:P V2

    decibel power ratios:10log10P2P1

  • 5/19/2018 01100_Freqresp

    29/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

  • 5/19/2018 01100_Freqresp

    30/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log

  • 5/19/2018 01100_Freqresp

    31/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log

    1 10 1001

    10

    100

    2

    (rad/s)

  • 5/19/2018 01100_Freqresp

    32/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.

    1 10 1001

    10

    100

    2

    (rad/s)

  • 5/19/2018 01100_Freqresp

    33/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.

    1 10 1001

    10

    100

    2

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc

  • 5/19/2018 01100_Freqresp

    34/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.

    1 10 1001

    10

    100

    2

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc

  • 5/19/2018 01100_Freqresp

    35/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.

    1 10 1001

    10

    100

    2

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc

  • 5/19/2018 01100_Freqresp

    36/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.

    1 10 1001

    10

    100

    2

    0.22

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc

  • 5/19/2018 01100_Freqresp

    37/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    1 10 1001

    10

    100

    2

    0.22

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc

  • 5/19/2018 01100_Freqresp

    38/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    1 10 1001

    10

    100

    2

    0.22

    80

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc

  • 5/19/2018 01100_Freqresp

    39/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    1 10 1001

    10

    100

    2

    0.22

    80

    65-1

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc

  • 5/19/2018 01100_Freqresp

    40/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    1 10 1001

    10

    100

    2

    0.22

    80

    65-1

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc 0, phase =90 magnitude slope.

    1 10 100-1

    -0.5

    0

    0.5

    1

    2 0.22

    80

    65-1

    (rad/s)

  • 5/19/2018 01100_Freqresp

    41/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    If |H| is measured in decibels, a slope ofris called6r dB/octaveor20r dB/decade.

    1 10 1001

    10

    100

    2

    0.22

    80

    65-1

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc 0, phase =90 magnitude slope.

    1 10 100-1

    -0.5

    0

    0.5

    1

    2 0.22

    80

    65-1

    (rad/s)

  • 5/19/2018 01100_Freqresp

    42/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    If |H| is measured in decibels, a slope ofris called6r dB/octaveor20r dB/decade.

    1 10 1001

    10

    100

    2

    0.22

    80

    65-1

    -9-1

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc 0, phase =90 magnitude slope.Negativec adds180 to the phase.

    1 10 100-1

    -0.5

    0

    0.5

    1

    2 0.22

    80

    65-1

    -9-1

    (rad/s)

  • 5/19/2018 01100_Freqresp

    43/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    Suppose we plot the magnitude and phase ofH=c (j)r

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    If |H| is measured in decibels, a slope ofris called6r dB/octaveor20r dB/decade.

    1 10 1001

    10

    100

    2

    0.22

    80

    65-1

    -9-1

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc 0, phase =90 magnitude slope.Negativec adds180 to the phase.

    Note:Phase angles are modulo360, i.e.450

    90. 1 10 100

    -1

    -0.5

    0

    0.5

    1

    2 0.22

    80

    65-1

    -9-1

    (rad/s)

  • 5/19/2018 01100_Freqresp

    44/118

    Logs of Powers

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 5 / 12

    H=c (j)r has a straight-line magnitude graph and a constant phase.

    Magnitude (log-log graph):

    |H| =cr log |H| = log |c|+r log This is a straight line with a slope ofr.conly affects the lines vertical position.

    If |H| is measured in decibels, a slope ofris called6r dB/octaveor20r dB/decade.

    1 10 1001

    10

    100

    2

    0.22

    80

    65-1

    -9-1

    (rad/s)

    Phase (log-lin graph):

    H= jr + c=r 2 (+ifc 0, phase =90 magnitude slope.Negativec adds180 to the phase.

    Note:Phase angles are modulo360, i.e.450

    90. 1 10 100

    -1

    -0.5

    0

    0.5

    1

    2 0.22

    80

    65-1

    -9-1

    (rad/s)

  • 5/19/2018 01100_Freqresp

    45/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

  • 5/19/2018 01100_Freqresp

    46/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    47/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    48/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1High frequencies ( 1RC):H(j) 1jRC

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    49/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1High frequencies ( 1RC):H(j) 1jRCApproximate the magnitude response

    as two straight lines

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    50/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 |H(j)| 1High frequencies ( 1RC):H(j) 1jRCApproximate the magnitude response

    as two straight lines

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    51/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 |H(j)| 1High frequencies ( 1RC):H(j) 1jRC |H(j)| 1RC1

    Approximate the magnitude response

    as two straight lines

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    52/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 |H(j)| 1High frequencies ( 1RC):H(j) 1jRC |H(j)| 1RC1

    Approximate the magnitude response

    as two straight lines

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    53/118

    Straight Line Approximations

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 |H(j)| 1High frequencies ( 1RC):H(j) 1jRC |H(j)| 1RC1

    Approximate the magnitude response

    as two straight lines intersecting at the

    corner frequency, c = 1RC.

    0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

  • 5/19/2018 01100_Freqresp

    54/118

    Straight Line Approximations

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 |H(j)| 1High frequencies ( 1RC):H(j) 1jRC |H(j)| 1RC1

    Approximate the magnitude response

    as two straight lines intersecting at the

    corner frequency, c = 1RC.

    At the corner frequency: 0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

    (a)the gradient changes by 1(= 6 dB/octave= 20 dB/decade).

  • 5/19/2018 01100_Freqresp

    55/118

    Straight Line Approximations

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 |H(j)| 1High frequencies ( 1RC):H(j) 1jRC |H(j)| 1RC1

    Approximate the magnitude response

    as two straight lines intersecting at the

    corner frequency, c = 1RC.

    At the corner frequency: 0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

    (a)the gradient changes by 1(= 6 dB/octave= 20 dB/decade).(b) |H(jc)| =

    11+j

    = 1

    2= 3 dB (worst-case error).

  • 5/19/2018 01100_Freqresp

    56/118

    Straight Line Approximations

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 6 / 12

    Key idea:(aj+ b)

    aj for |a| |b|b for |a| |b|

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 |H(j)| 1High frequencies ( 1RC):H(j) 1jRC |H(j)| 1RC1

    Approximate the magnitude response

    as two straight lines intersecting at the

    corner frequency, c = 1RC.

    At the corner frequency: 0.1/RC 1/RC 10/RC-30

    -20

    -10

    0

    (rad/s)

    |Gain|(dB)

    (a)the gradient changes by 1(= 6 dB/octave= 20 dB/decade).(b) |H(jc)| =

    11+j

    = 1

    2= 3 dB (worst-case error).

    A linear factor(aj+ b)has a corner frequency ofc = ba .

  • 5/19/2018 01100_Freqresp

    57/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)

  • 5/19/2018 01100_Freqresp

    58/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)

  • 5/19/2018 01100_Freqresp

    59/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)

  • 5/19/2018 01100_Freqresp

    60/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50Step 3:For

  • 5/19/2018 01100_Freqresp

    61/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50Step 3:For

  • 5/19/2018 01100_Freqresp

    62/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50Step 3:For

  • 5/19/2018 01100_Freqresp

    63/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50Step 3:For

  • 5/19/2018 01100_Freqresp

    64/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50Step 3:For

  • 5/19/2018 01100_Freqresp

    65/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50Step 3:For

  • 5/19/2018 01100_Freqresp

    66/118

    Plot Magnitude Response

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 7 / 12

    The gain of a linear circuit is always arational polynomial inj and iscalled thetransfer functionof the circuit. For example:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Sort corner freqs:1, 4, 12, 50Step 3:For

  • 5/19/2018 01100_Freqresp

    67/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    L d Hi h F A t t

  • 5/19/2018 01100_Freqresp

    68/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)0.1 1 10 100 1000

    -0.5

    0

    0.5

    (rad/s)

    Low and High Frequency Asymptotes

  • 5/19/2018 01100_Freqresp

    69/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)0.1 1 10 100 1000

    -0.5

    0

    0.5

    (rad/s)

    Low Frequency Asymptote:

    Low and High Frequency Asymptotes

  • 5/19/2018 01100_Freqresp

    70/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)0.1 1 10 100 1000

    -0.5

    0

    0.5

    (rad/s)

    Low Frequency Asymptote:From factors:HLF(j) =

    20j(12)(1)(4)(50) = 1.2j

    Low and High Frequency Asymptotes

  • 5/19/2018 01100_Freqresp

    71/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)0.1 1 10 100 1000

    -0.5

    0

    0.5

    (rad/s)

    Low Frequency Asymptote:From factors:HLF(j) =

    20j(12)(1)(4)(50) = 1.2j

    Lowestpower ofj on top and bottom:H(j) 720(j)600 = 1.2j

    Low and High Frequency Asymptotes

  • 5/19/2018 01100_Freqresp

    72/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)0.1 1 10 100 1000

    -0.5

    0

    0.5

    (rad/s)

    Low Frequency Asymptote:From factors:HLF(j) =

    20j(12)(1)(4)(50) = 1.2j

    Lowestpower ofj on top and bottom:H(j) 720(j)600 = 1.2jHigh Frequency Asymptote:

    Low and High Frequency Asymptotes

  • 5/19/2018 01100_Freqresp

    73/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)0.1 1 10 100 1000

    -0.5

    0

    0.5

    (rad/s)

    Low Frequency Asymptote:From factors:HLF(j) =

    20j(12)(1)(4)(50) = 1.2j

    Lowestpower ofj on top and bottom:H(j) 720(j)600 = 1.2jHigh Frequency Asymptote:

    From factors:HHF(j) = 20j(j)(j)(j)(j) = 20 (j)

    1

    Low and High Frequency Asymptotes

  • 5/19/2018 01100_Freqresp

    74/118

    Low and High Frequency Asymptotes

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 8 / 12

    You can find the low and high frequency asymptotes without factorizing:

    H(j) = 60(j)2+720(j)

    3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    0.1 1 10 100 1000

    -40

    -20

    0

    (rad/s)0.1 1 10 100 1000

    -0.5

    0

    0.5

    (rad/s)

    Low Frequency Asymptote:From factors:HLF(j) =

    20j(12)(1)(4)(50) = 1.2j

    Lowestpower ofj on top and bottom:H(j) 720(j)600 = 1.2jHigh Frequency Asymptote:

    From factors:HHF(j) = 20j(j)(j)(j)(j) = 20 (j)

    1

    Highestpower ofj on top and bottom:H(j) 60(j)23(j)3

    = 20(j)1

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    75/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    76/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    77/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    1 = 0

    0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    78/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    1 = 0

    High frequencies ( 1RC):H(j) 1jRC

    0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    79/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    1 = 0

    High frequencies ( 1RC):H(j) 1jRC j1 = 2

    0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    80/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    1 = 0

    High frequencies ( 1RC):H(j) 1jRC j1 = 2Approximate the phase response as

    three straight lines.

    0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    81/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High Frequency

    Asymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    1 = 0

    High frequencies ( 1RC):H(j) 1jRC j1 = 2Approximate the phase response as

    three straight lines.

    By chance, they intersect close to

    0.1c and10c wherec= 1RC. 0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    82/118

    Phase Approximation

    11: Frequency Responses Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    1 = 0

    High frequencies ( 1RC):H(j) 1jRC j1 = 2Approximate the phase response as

    three straight lines.

    By chance, they intersect close to

    0.1c and10c wherec= 1RC. 0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Between0.1c and10c the phase changes by

    2over two decades.

    This gives a gradient = 4 radians/decade.

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    83/118

    ase pp o at o

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j)

    1

    1 = 0

    High frequencies ( 1RC):H(j) 1jRC j1 = 2Approximate the phase response as

    three straight lines.

    By chance, they intersect close to

    0.1c and10c wherec= 1RC. 0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Between0.1c and10c the phase changes by

    2over two decades.

    This gives a gradient = 4 radians/decade.(aj+ b)in denominator gradient= 4 /decade at

    = 101ba .

    Phase Approximation

  • 5/19/2018 01100_Freqresp

    84/118

    pp

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 9 / 12

    Gain:H(j) = 1jRC+1

    Low frequencies ( 1RC):H(j) 1 1 = 0

    High frequencies ( 1RC):H(j) 1jRC j1 = 2Approximate the phase response as

    three straight lines.

    By chance, they intersect close to

    0.1c and10c wherec= 1RC. 0.1/RC 1/RC 10/RC

    -0.4

    -0.2

    0

    (rad/s)

    Phas

    e/

    Between0.1c and10c the phase changes by

    2over two decades.

    This gives a gradient = 4 radians/decade.(aj+ b)in denominator gradient= 4 /decade at

    = 101ba .

    The sign ofgradient is reversed for (a) numerator factors and (b) ba

  • 5/19/2018 01100_Freqresp

    85/118

    p

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    86/118

    p

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    87/118

    p

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    88/118

    p

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    89/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    90/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    91/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    92/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    93/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48) 1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .Step 7:At

    = 1.2,= 0.35 0.48

    2 = 0.11. New gradient is

    4.

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    94/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62) 5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .Step 7:At

    = 1.2,= 0.35 0.48

    2 = 0.11. New gradient is

    4.

    Steps 8-12:Repeat for each gradient change.

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    95/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3) 10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .Step 7:At

    = 1.2,= 0.35 0.48

    2 = 0.11. New gradient is

    4.

    Steps 8-12:Repeat for each gradient change.

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    96/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 =

    20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6) 40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .Step 7:At = 1.2,= 0.35

    0.48

    2 = 0.11. New gradient is

    4.

    Steps 8-12:Repeat for each gradient change.

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    97/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 = 20

    j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .Step 7:At = 1.2,= 0.35

    0.48

    2 = 0.11. New gradient is

    4.

    Steps 8-12:Repeat for each gradient change.

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    98/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40+

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .Step 7:At = 1.2,= 0.35

    0.48

    2 = 0.11. New gradient is

    4.

    Steps 8-12:Repeat for each gradient change. Final gradient is always 0.

    Plot Phase Response

  • 5/19/2018 01100_Freqresp

    99/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers

    Straight Line

    Approximations

    Plot Magnitude Response

    Low and High FrequencyAsymptotes

    Phase Approximation

    Plot Phase Response

    RCR Circuit

    Summary

    E1.1 Analysis of Circuits (2014-5225) Frequency Responses: 11 10 / 12

    H(j) = 60(j)2

    +720(j)3(j)3+165(j)2+762(j)+600 = 20j(j+12)(j+1)(j+4)(j+50)

    Step 1:Factorize the polynomials

    Step 2:Gradient changes at101c.

    Sign depends on num/den and sgnba

    :.1, 10+; .4, 40+; 1.2+, 120; 5, 500+

    0.1 1 10 100 1000-0.5

    0

    0.5

    (rad/s)

    Step 3:Put in ascending order and calculate gaps aslog1012

    decades:

    .1 (.6) .4 (.48)1.2+

    (.62)5 (.3)10+

    (.6)40

    +

    (.48) 120 (.62) 500+

    .Step 4:Find phase of LF asymptote: 1.2j= +2 .Step 5:At = 0.1gradient becomes 4 .is still 2 .Step 6:At = 0.4,= 2 0.64 = 0.35. New gradient is 2 .Step 7:At = 1.2,= 0.35

    0.48

    2 = 0.11. New gradient is

    4.

    Steps 8-12:Repeat for each gradient change. Final gradient is always 0.

    At 0.1 and 10 times each corner frequency, the graph is continuous but its

    gradient changes abruptly by 4 rad/decade.

    RCR Circuit

  • 5/19/2018 01100_Freqresp

    100/118

    11: Frequency Responses

    Frequency Response

    Sine Wave Response

    Logarathmic axes

    Logs of Powers