ECE 1311 Ch11

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    ECE 1311

    Chapter 11AC PowerAnalysis

    1

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    Outlines

    11.1 Instantaneous and Average Power11.2 Maximum Average Power Transfer

    11.3 Effective or RMS Value11.4 Apparent Power and Power Factor11.5 Complex Power

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    Sinusoidal power at 2tConstant power

    )2(cos2

    1

    )(cos2

    1

    )(cos)(cos)()()(

    ivmmivmm

    ivmm

    tIVIV

    ttIVtitvtp

    w

    ww

    11.1 Instantaneous andAverage Power (1)

    The instantaneous power (p(t))

    p(t) > 0: power is absorbed by the circuit; p(t) < 0: power is supplied by the circuit.

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    )(cos2

    1)(

    1

    0ivmm

    T

    IVdttpT

    P

    11.1 Instantaneous andAverage Power (2)

    The average power (P) is the average of the instantaneouspower over one period.

    1. P is not time dependent.

    2. When v= i , it is a purely

    resistiveload case.

    3. When vi= 90o, it is a

    purely reactiveload case.

    4. P = 0 means that the circuit

    absorbs no average power.

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    )6010(sin15)(

    )2010(cos80)(

    tti

    ttv

    11.1 Instantaneous andAverage Power (3)

    Example 1

    Calculate the instantaneous power and average

    power absorbed by a passive linear network if:

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    Example 2

    A current flows through an

    impedance . Find the average

    power delivered to the impedance.

    11.1 Instantaneous andAverage Power (4)

    3010I

    2220 Z

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    Example 3

    Calculate the average power absorbed by the resistor and

    inductor. Find the average power supplied by the voltage

    source.

    11.1 Instantaneous andAverage Power (5)

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    11.2 Maximum Average PowerTransfer (1)

    The maximum average power

    can be transferred to the load if:

    TH

    2

    TH

    maxR8

    VP

    If the load is purely real, then:TH

    2

    TH

    2

    THL ZXRR

    *ThL ZZ

    L

    2

    max RI

    2

    1P

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    11.2 Maximum Average PowerTransfer (2)

    Example 4

    For the circuit shown below, find the load impedance ZLthatabsorbs the maximum average power. Calculate that maximum

    average power.

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    11.3 Effective or RMS Value (1)

    2

    II mrms

    The average power can be written in terms of

    the rms values:

    )(cosIV)(cosIV2

    1

    ivrmsrmsivmm P

    Note: If you express amplitude of a phasor source(s) in rms, then all the

    answers as a result of this phasor source(s) must also be in rms value.

    The rms value of a sinusoid i(t) = Imcos(wt)is given by:

    rmseff II--Note

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    11.4 Apparent Power andPower Factor (1)

    Apparent Power (S)is the product of the rms values ofvoltage and current.

    It is measured in volt-amperesor VA to distinguish it fromthe average or real power which is measured in watts.

    Power factor is: the cosine of the phase difference between the voltage and current

    or

    The cosine of the angle of the load impedance.

    )(cosS)(cosIVP ivivrmsrms

    Apparent Power, S Power Factor, pf

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    11.4 Apparent Power andPower Factor (2)

    Purely resistive

    load (R)vi = 0, pf = 1 P/S = 1, all power are

    consumed

    Purely reactive

    load (L or C)vi = 90

    o,

    pf = 0

    P = 0, no real power

    consumption

    Resistive and

    reactive load

    (R and L/C)

    vi > 0

    vi < 0

    Lagging- inductive

    load

    Leading- capacitive

    load

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    11.4 Apparent Power andPower Factor (3)

    Example 5

    For the circuit shown below, calculate the power factor as seenby the voltage source. What is the average power supplied by

    the voltage source?

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    11.5 Complex Power (1)

    Complex power (S) is the product of the voltage and the

    complex conjugate of the current:

    *IVIV2

    1S

    rmsrms

    *Z

    VZIS

    2

    rms2

    rms

    imvm IV IV

    irmsvrms IV IV

    Note:

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    11.5 Complex Power (2)

    ivrmsrms IVIV2

    1S

    )(sinIVj)(cosIVS ivrmsrmsivrmsrms

    P: is the average power in wattsdelivered to a load and it is the only useful

    power.

    Q: is the reactive power exchangebetween the source and

    the reactive part of the load. It is measured in volt-ampere-reactive (VAR).

    Q = 0 for resistive loads(unity pf).

    Q < 0 for capacitive loads(leading pf).

    Q > 0 for inductive loads(lagging pf).

    S = P + j Q

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    11.5 Complex Power (3)

    )(sinIVj)(cosIVS ivrmsrmsivrmsrms

    Apparent Power:S = |S| = Vrms*Irms=

    Real power: P = Re(S) = S cos(vi)

    Reactive Power: Q = Im(S) = S sin(vi)

    Power factor: pf = P/S = cos(vi)

    S = P + j Q

    22 QP

    S

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    11.5 Complex Power (4)

    )(sinIVj)(cosIVS ivrmsrmsivrmsrms

    S = P + j Q

    Impedance TrianglePower Factor

    Power Triangle

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    11.5 Complex Power (5)

    Example 6:

    Given:

    Determine:

    The complex and apparent powers.

    The real and reactive powers.

    The power factor and the load impedance.

    AI

    VV

    rms

    rms

    154.0

    85110