Chapter 1 0 - RC Circuits - I-Shou University - 義守大學 · PDF fileThe frequency response of the low-pass RC circuit is shown below, where the measured values are plotted on a

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  • ISU EE C.Y. Lee

    Chapter 10RC Circuits

  • 2ISU EE C.Y. Lee

    ObjectivesDescribe the relationship between current and voltage in an RC circuitDetermine impedance and phase angle in a seriesRC circuitAnalyze a series RC circuitDetermine the impedance and phase angle in a parallel RC circuitAnalyze a parallel RC circuit Analyze series-parallel RC circuitsDetermine power in RC circuits

  • 3ISU EE C.Y. Lee

    Sinusoidal Response of RC Circuits

    The capacitor voltage lags the source voltage Capacitance causes a phase shift between voltageand current that depends on the relative values of the resistance and the capacitive reactance

  • 4ISU EE C.Y. Lee

    Impedance and Phase Angle of Series RC Circuits

    The phase angle is the phase difference between the total current and the source voltageThe impedance of a series RC circuit is determined by both the resistance (R) and the capacitive reactance (XC)

    (Z = RjXC)(Z = jXC)(Z = R)

    (ZC= 1/jC= jXC) (Z= R+ZC= RjXC)

  • 5ISU EE C.Y. Lee

    Impedance and Phase Angle of Series RC Circuits

    In the series RC circuit, the total impedance is the phasor sum of R and jXCImpedance magnitude: Z = R2 + X2CPhase angle: = tan-1(XC/R)

  • 6ISU EE C.Y. Lee

    Impedance and Phase Angle of Series RC Circuits

    Z = (47)2 + (100)2 = 110 = tan-1(100/47) = tan-1(2.13) = 64.8

    Example: Determine the impedance and the phase angle

  • 7ISU EE C.Y. Lee

    Analysis of Series RC Circuits

    The application of Ohms law to series RC circuits involves the use of the quantities Z, V, and I as:

    IZV =

    ZVI =

    IVZ =

  • 8ISU EE C.Y. Lee

    Analysis of Series RC CircuitsExample: If the current is 0.2 mA, determine the source

    voltage and the phase angle

    XC = 1/2(1103)(0.0110-6) = 15.9 kZ = (10103)2 + (15.9103)2 = 18.8 kVS = IZ = (0.2mA)(18.8k) = 3.76 V = tan-1(15.9k/10k) = 57.8

  • 9ISU EE C.Y. Lee

    Relationships of I and V in a Series RC Circuit

    In a series circuit, the current is the same through both the resistor and the capacitorThe resistor voltage is in phase with the current, and the capacitor voltage lags the current by 90

    I

    VR

    VC

    VS

  • 10ISU EE C.Y. Lee

    KVL in a Series RC Circuit

    From KVL, the sum of the voltage drops must equal the applied voltage (VS)

    Since VR and VC are 90out of phase with each other, they must be added as phasor quantities

    VS = V2R + V2C = tan-1(VC/VR)

    VR

    VC

    VS

    I

    VR= IR

    VS= IZ = I(RjXC)VC= I(jXC)

  • 11ISU EE C.Y. Lee

    KVL in a Series RC CircuitExample: Determine the source voltage and the phase angle

    VS = (10)2 + (15)2 = 18 V = tan-1(15/10) = tan-1(1.5) = 56.3

  • 12ISU EE C.Y. Lee

    Variation of Impedance and Phase Angle with Frequency

    For a series RC circuit; as frequency increases: R remains constant XC decreases Z decreases decreases

    f Z

    R

  • 13ISU EE C.Y. Lee

    Variation of Impedance and Phase Angle with Frequency

    Example: Determine the impedance and phase angle for each of the following values of frequency: (a) 10 kHz (b) 30 kHz

    (a)XC = 1/2(10103)(0.0110-6) = 1.59 kZ = (1.0103)2 + (1.59103)2 = 1.88 k = tan-1(1.59k/1.0k) = 57.8

    (b)XC = 1/2(30103)(0.0110-6) = 531 kZ = (1.0103)2 + (531)2 = 1.13 k = tan-1(531/1.0k) = 28.0

  • 14ISU EE C.Y. Lee

    Impedance and Phase Angle of Parallel RC Circuits

    Total impedance in parallel RC circuit:Z = (RXC) / ( R2 +X2C)

    Phase angle between the applied V and the total I: = tan-1(R/XC)

    ( )

    jRXRXZ

    jXRRjX

    Z

    jXRZ

    C

    C

    C

    C

    C

    +=

    +

    =

    +=

    1

    111

    +

    ==jRX

    RXIIZVC

    C

  • 15ISU EE C.Y. Lee

    Conductance, Susceptance and Admittance

    Conductance is the reciprocal of resistance:G = 1/R

    Capacitive susceptance is the reciprocal of capacitive reactance:

    BC = 1/XCAdmittance is the reciprocal of impedance:

    Y = 1/Z

  • 16ISU EE C.Y. Lee

    Ohms Law

    Application of Ohms Law to parallel RC circuits using impedance can be rewritten for admittance (Y=1/Z):

    YIV =

    VYI =

    VIY =

  • 17ISU EE C.Y. Lee

    Relationships of the I and V in a Parallel RC Circuit

    The applied voltage, VS, appears across both the resistive and the capacitive branchesTotal current, Itot, divides at the junction into the two branch current, IR and IC

    Vs, VR, VC

    IR= V/R

    Itot= V/Z = V((XC+jR)/RXC)IC= V/(jXC)

  • 18ISU EE C.Y. Lee

    KCL in a Parallel RC Circuit

    From KCL, Total current (IS) is the phasor sum of the two branch currents

    Since IR and IC are 90out of phase with each other, they must be added as phasor quantities

    Itot = I2R + I2C = tan-1(IC/IR)

    IR= V/R

    Itot= V/Z = V((XC+jR)/RXC)IC= V/(jXC)

  • 19ISU EE C.Y. Lee

    KCL in a Parallel RC CircuitExample: Determine the value of each current, and describe

    the phase relationship of each with the source voltage

    IR = 12/220 = 54.5 mAIC = 12/150 = 80 mAItot = (54.5)2 + (80)2 = 96.8 mA = tan-1(80/54.5) = 55.7

    Vs

  • 20ISU EE C.Y. Lee

    Series-Parallel RC CircuitsAn approach to analyzing circuits with combinations of both series and parallel R and C elements is to: Calculate the magnitudes of capacitive reactances (XC) Find the impedance (Z) of the series portion and the

    impedance of the parallel portion and combine them to get the total impedance

  • 21ISU EE C.Y. Lee

    (Z)(Z')(Z"):

    Z= Z' jZ"

    ( )mi jXRRZ ++=

    111

    ( ) 22222

    mie

    meieie

    XRRXRRRRRZ

    ++++

    =

    ( ) 222

    mie

    me

    XRRXRj++

  • 22ISU EE C.Y. Lee

  • 23ISU EE C.Y. Lee

    c c

    Z-plot

    Z:

    Zs:

    fC ():Z"

    ( ) ( )22 ZZZ +=

  • 24ISU EE C.Y. Lee

    Z-plot

  • 25ISU EE C.Y. Lee

    RC Lag NetworkThe RC lag network is a phase shift circuit in which the output voltage lags the input voltage

    =

    RXC1tan90o

  • 26ISU EE C.Y. Lee

    RC Lead NetworkThe RC lead network is a phase shift circuit in which the output voltage leads the input voltage

    =

    RXC1tan

  • 27ISU EE C.Y. Lee

    Frequency Selectivity of RC CircuitsA low-pass circuit is realized by taking the output across the capacitor, just as in a lag network

  • 28ISU EE C.Y. Lee

    Frequency Selectivity of RC CircuitsThe frequency response of the low-pass RC circuit is shown below, where the measured values are plotted on a graph of Vout versus f.

    10 V

  • 29ISU EE C.Y. Lee

    Frequency Selectivity of RC CircuitsA high-pass circuit is implemented by taking the output across the resistor, as in a lead network

  • 30ISU EE C.Y. Lee

    Frequency Selectivity of RC CircuitsThe frequency response of the high-pass RC circuit is shown below, where the measured values are plotted on a graph of Vout versus f.

    10 V

  • 31ISU EE C.Y. Lee

    Frequency Selectivity of RC CircuitsThe frequency at which the capacitive reactance equals the resistance in a low-pass or high-pass RC circuit is called the cutoff frequency:

    RCfC 2

    1=

  • 32ISU EE C.Y. Lee

    Coupling an AC Signal into a DC Bias Network

  • 33ISU EE C.Y. Lee

    Summary

    When a sinusoidal voltage is applied to an RC circuit, the current and all the voltage drops are also sine wavesTotal current in an RC circuit always leads the source voltageThe resistor voltage is always in phase with the currentIn an ideal capacitor, the voltage always lags the current by 90

  • 34ISU EE C.Y. Lee

    Summary

    In an RC circuit, the impedance is determined by both the resistance and the capacitive reactance combinedThe circuit phase angle is the angle between the total current and the source voltageIn a lag network, the output voltage lags the input voltage in phaseIn a lead network, the output voltage leads the input voltageA filter passes certain frequencies and rejects others

    Chapter 10ObjectivesSinusoidal Response of RC CircuitsImpedance and Phase Angle of Series RC CircuitsImpedance and Phase Angle of Series RC CircuitsAnalysis of Series RC CircuitsAnalysis of Series RC CircuitsRelationships of I and V in a Series RC CircuitKVL in a Series RC CircuitKVL in a Series RC CircuitVariation of Impedance and Phase Angle with FrequencyVariation of Impedance and Phase Angle with FrequencyImpedance and Phase Angle of Parallel RC CircuitsConductance, Susceptance and AdmittanceOhms LawRelationships of the I and V in a Parallel RC CircuitKCL in a Parallel RC CircuitKCL in a Parallel RC CircuitSeries-Parallel RC CircuitsRC Lag NetworkRC Lead NetworkFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsFrequency Selectivity of RC CircuitsCoupling an AC Signal into a DC Bias NetworkSummarySummary