frequency selective networks

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    Frequency selectivenetworks

    There are man frequency selectivenetworks, the most common twonetworks are the series and parallel

    resonant circuits

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    Series resonant circuit

    In this kind ofcircuits, at theresonant frequencythe inductor and

    capacitors has equalimpedances withopposite signs

    At the resonantfrequency vO will bein phase with vi

    The quality factor forthis circuit is givenby

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    Series resonant circuit

    The quality factor gives an indication ofthe bandwidth of the circuit

    Narrower bandwidth means that the

    circuit has a larger quality factor as shownin the Figure

    f1

    f2

    3-dB

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    Series resonant circuit

    The quality factor is dened according tothe following equation

    The bandwidth is dened as the dierencebetween f1and f2

    At these two particular frequencies thesignal amplitude is less by ! d" asindicated by the gure in slide !

    B

    Q O

    =

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    Series resonant circuitexample

    Example:#esign a lter to couple a voltagesource, with negligible source impedance,to a $% ohm load resistance& The

    specications are that the lter centerfrequency be $ '() and the bandwidth be*%% k()

    Solution

    From the quality factor we nd thatH

    B

    RL

    6.79

    102

    505 =

    ==

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    Series resonant circuitexample

    Solution

    The capacitance value can be found from

    LCf

    2

    10=

    ( ) ( ) ( ) FLfC =

    == 7.12106.791052

    1

    2

    1

    625220

    2

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    Series resonant circuit

    The circuit gain at any frequency can bedetermined from

    The attenuation at any harmonic can befound from

    22 )1(

    /

    )(O

    n

    LRn

    jnA

    O

    O

    =

    )1()(

    )(2

    =nQ

    n

    jA

    jnA

    O

    O

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    Series resonant circuitexample

    Example: A series tuned circuit is to be used tolter out harmonics of a waveform& +hat mustbe the minimum for the amplitude of the fthharmonic to be -% d" below the amplitude of

    the fundamental frequencySolution

    -% d" corresponds to a voltage ratio of *%%.*, n/$

    This means that /0%&1!)15(

    501.0)5(2

    ==Q

    jA O

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    Parallel resonant circuit

    In parallel resonant circuit twosusceptances are added in parallel, sothat the admittance, instead of impedance

    is a minimum at fO

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    Parallel resonant circuit

    In practical life the inductor usually has anite resistance, therefore a moreaccurate model for the parallel resonant

    circuit is shown below

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    Impedance matching andharmonic fltering using

    reactive networks 2eactive networks can be used to matchimpedances over a narrow frequencyrange

    These networks can also be used to lterout some harmonics

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    Impedance matching

    The input impedance of the two networksshown in the ne3t slide are equal provided

    If we take the real and imaginary partsand equate them we get the following

    22

    2

    22

    2

    pp

    pp

    pp

    pp

    pp

    pp

    ssiXR

    XR

    jXR

    XR

    jXR

    jXR

    jXRZ ++=

    ==

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    Impedance matching

    The previous equations can be rewrittenas

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    Impedance matching

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    Impedance matching andharmonic fltering using

    reactive networksExample. The input impedance of a transistoramplifier is equal to *% 4 in series with %&05(& #esign a matching network so that theinput impedance is $% 4 at 0% '()

    Solution:

    At 0% '() the inductive reactance of a %&0 5(inductor is 0$&* 4& The combined impedanceof the circuit became *%670$&* 4&

    To do the impedance transformation we canuse the equation

    s

    ssp

    R

    XRR

    22+

    =

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    I d t hi d

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    Impedance matching andharmonic fltering using

    reactive networksSolution:8r

    in order to convert the real part of theimpedance to $% 4, the imaginary partbecameXs=20 4&

    In order to convert the 0$&* 4 to 0% 4 aseries reactance of 9j5.1 4 must beadded to the circuit&

    10

    1050

    22

    sX+= 201001050 ==sX

    fcj

    j2

    11.5 = nFc 56.1=

    I d t hi d

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    Impedance matching andharmonic fltering using

    reactive networksSolution:NowXpcan be found from

    if a reactance of j25 is added in parallelwith the circuit as shown in the gure of

    the ne3t slide then input impedancebecame e3actly $% 4The :70$ reactance results from the

    impedance of a capacitor !*1 pF

    s

    ss

    p X

    XRjjX

    22+

    = =+

    = 25

    20

    2010 22

    jjjXp

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    I d t hi d

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    Impedance matching andharmonic fltering using

    reactive networksExample. #esign a lossless matchingnetwork to couple the impedance shownin the fig& below to a $% ; sourceimpedance at 0% '()

    I d t hi d

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    Impedance matching andharmonic fltering using

    reactive networkssolution.

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    Impedance matching andharmonic fltering using

    reactive networksSolution.

    The input impedance of the circuit is

    This can be brought to $% ; only by adding a

    j50 ; reactance in series with the abovementioned circuit&

    The completed solution will similar to the oneshown in the ne3t circuit

    5050 jZi +=

    I d t hi d

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    Impedance matching andharmonic fltering using

    reactive networks