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Lec 3

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  • Outline

    Review

    1/21/2015

    Summary

    Single time Constant (STC) Networks

    Voltage Amplifiers

    Frequency Response of Amplifiers

    Outline

    1

    Single time Constant (STC) Networks

    Frequency Response of Amplifiers

  • Review

    1/21/2015

    Amplifier Saturation

    Circuit Models for Amplifiers

    NonLinear Transfer Characterstics(T.F) and Biasing

    Review

    2

    Circuit Models for Amplifiers

    NonLinear Transfer Characterstics(T.F) and

  • Different Types of Amplifiers

    Voltage Amplifier

    Current Amplifier

    TransConductance Amplifier

    TransResistance Amplifier

    Different Types of Amplifiers

    Amplifier

    Amplifier

  • Voltage Amplifier

    1/21/2015 EEE C424/ECE C313

    Voltage Amplifier

    EEE C424/ECE C313 4

    Input resistance RiOutput resitance R0Open circuit voltage gain AVo

  • Voltage Amplifier (Input section)

    1/21/2015 EEE C424/ECE C313

    Voltage Amplifier (Input section)

    EEE C424/ECE C313 5

  • Inorder not to lose a significant portion of the input signal in coupling the signal source to the amplifier input ,the amplifier must be designed to have input resistance Rgreater than Rs

    1/21/2015 EEE C424/ECE C313

    Voltage Amplifier (Input section)

    Inorder not to lose a significant portion of the input signal in coupling the signal source to the amplifier input ,the amplifier must be

    input resistance Ri must

    EEE C424/ECE C313 6

    Voltage Amplifier (Input section)

  • Voltage Amplifier (Input section)

    1/21/2015 EEE C424/ECE C313

    Voltage Amplifier (Input section)

    EEE C424/ECE C313 7

  • Voltage Amplifier (Input section)

    1/21/2015 EEE C424/ECE C313

    Ri >> Rs

    Voltage Amplifier (Input section)

    EEE C424/ECE C313 8

  • 1/21/2015 EEE C424/ECE C313

    Voltage Amplifier (Output section)

    EEE C424/ECE C313 9

    Voltage Amplifier (Output section)

  • Voltage Amplifier (Output section)

    Using voltage divider rule

    Voltage Gain is given by

    Voltage Amplifier (Output section)

    Using voltage divider rule

  • Voltage Gain is given by

    Inorder not to lose gain in couplingto a load, the output resistancethan the load resistance RL

    Ro

  • Overall voltage Gain vousing

    o /vs can be found by

  • Frequency Response of Amplifiers

    A linear amplifier fed at its input with a sinewave signal Vi and frequency

    1/21/2015

    Frequency Response of Amplifiers

    A linear amplifier fed at its input with a sine-and frequency

    13

  • Frequency Response of Amplifiers

    Whenever a sine-wave signal is applied to a linear circuit ,the resulting output is sinusiodal with the same frequency as the input

    The output sinusoid will have different amplitude and will be shifted in phase relative to the input

    1/21/2015

    Frequency Response of Amplifiers

    wave signal is applied to a linear circuit ,the resulting output is sinusiodal with the same frequency as the input

    The output sinusoid will have different amplitude and will be shifted in phase relative

    14

  • Two plots w.r.t frequency on X

    Magnitude plot Phase plot

    This plots together called as

    1/21/2015 EEE C44/ECE C313

    Frequency Response of Amplifiers

    Two plots w.r.t frequency on X-axis

    This plots together called as Bode plots

    EEE C44/ECE C313 15

    Frequency Response of Amplifiers

  • Magnitude plot

    1/21/2015 EEE C44/ECE C313

    Magnitude plot

    EEE C44/ECE C313 16

  • Phase Plot

    Phase plot

    1/21/2015 EEE C44/ECE C313

    Phase Plot

    EEE C44/ECE C313 17

  • Amplifier Bandwidth

    1/21/2015

    Amplifier Bandwidth

    18

  • STC Networks

    An STC network is onecan be reduced to, one

    (capacitance or inductance) and one resistance

    An STC network formed by of an and a resistance R has a time constant

    1/21/2015

    STC Networks

    one that is composed of ,orone reactive component

    (capacitance or inductance) and one resistance

    An STC network formed by of an capacitance Chas a time constant =CR

    19

  • STC Networks

    An STC network formed by of an capacitance C and a resistance R has a time constant

    1/21/2015

    STC Networks

    An STC network formed by of an capacitance C and a resistance R has a time constant =CR

    20

  • STC Networks

    An STC network formed by of an and a resistance R has a time constant

    1/21/2015 EEE C424/ECE C313

    STC Networks

    An STC network formed by of an inductance Lhas a time constant =L/R

    EEE C424/ECE C313 21

  • STC Networks

    Most STC networks can be classified into two categories

    Low Pass Filter High Pass Filter

    1/21/2015

    STC Networks

    Most STC networks can be classified into two

    22

  • lowpasslowpass

    bandpassbandpass

    STC Networks

    highpasshighpass

    bandstopbandstop

    STC Networks Filters (ideal)

  • lowpasslowpass

    bandpassbandpass

    STC Networks Filters (

    bandstopbandstop

    highpasshighpass

    Filters (RealisticRealistic)

  • STC Networks

    This passes low frequency sine wave inputs with little or no attenuation at w= 0

    Attenuates the high frequency input sinusoids This is a Low pass Filter1/21/2015

    STC Networks

    This passes low frequency sine wave inputs with little or no attenuation at w= 0

    Attenuates the high frequency input sinusoids

    a Low pass Filter25

  • STC Networks

    This attenuates low frequency sine wave inputs with little or no attenuation at w= 0

    Passes the high frequency input sinusoids This is a High pass Filter

    1/21/2015

    STC Networks

    This attenuates low frequency sine wave inputs with little or no attenuation at w= 0

    Passes the high frequency input sinusoids

    a High pass Filter

    26

  • Consider the circuit below.

    R

    CVI

    +

    _

    1( )

    1( ) 1OV jw jwC

    V jw jwRCRi jwC

    Low pass filter circuit

    Low Pass FilterConsider the circuit below.

    C VO

    +

    _

    1( ) 1V jw jwRC

    Low pass filter circuit

    Low Pass Filter

  • 1( )

    1( ) 1OV jw jwC

    V jw jwRCRi jwC

    Low Pass Passive Filter

    jSubstituting

    1( ) 1V jw jwRC

    Low Pass Passive Filter

    = s

  • Low Pass Passive Filter

    Substituting

    0 = Corner Frequency

    Low Pass Passive Filter

    0 = 1 / RC

    = Corner Frequency

  • 1/21/2015

    Design Low pass Filtercutoff frequency 150Hz

    Filter for sub woofer withHz

  • Consider the circuit below.

    C

    RVi+

    _

    ( )1( ) 1

    OV jw jwRCRV jw jwRCRi jwC

    High Pass Filter

    High Pass Passive Filter

    Consider the circuit below.

    VO

    +

    _

    1( ) 1V jw jwRCRV jw jwRC

    jwC

    High Pass Filter

    High Pass Passive Filter

  • ( )1( ) 1

    OV jw jwRCRV jw jwRCRi jwC

    High Pass Passive Filter

    jSubstituting

    ( ) 1V jw jwRCV jw jwRC

    High Pass Passive Filter

    = s

  • High Pass Passive Filter

    Substituting

    0 = Corner Frequency

    High Pass Passive Filter

    0 = 1 / RC

    = Corner Frequency

  • 1/21/2015

    Active Filter

    Active Element

    BJTAmplifier

    MOS Amplifier 34

    Active Filter

    Active Element

    MOS Amplifier

    OPAMP Amplifier

  • Frequency response of STC networks

    1/21/2015

    Frequency response of STC networks

    35

  • Frequency response of STC networks

    1/21/2015

    Frequency response of STC networks

    36

  • ExampleExample

    Original signal

    Low-pass filtered

    High-pass filtered

    Band-pass filtered

    Band-stop filtered


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