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    14: Power in AC Circuits

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 1 / 11

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)50 100 150 200 250

    0

    0.5

    1

    t (s)

    2

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)50 100 150 200 250

    0

    0.5

    1

    t (s)

    2

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

    Average Powerdissipated inR:

    P = 1

    T T

    0 p(t)dt

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)50 100 150 200 250

    0

    0.5

    1

    t (s)

    2

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

    Average Powerdissipated inR:

    P = 1

    T T

    0 p(t)dt = 1

    R 1

    T T

    0 v2

    (t)dt

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)50 100 150 200 250

    0

    0.5

    1

    t (s)

    2

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

    Average Powerdissipated inR:

    P = 1

    T T

    0 p(t)dt = 1

    R 1

    T T

    0 v2

    (t)dt =v2

    R

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)50 100 150 200 250

    0

    0.5

    1

    t (s)

    2 v2(t)

    mean(v2)

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

    Average Powerdissipated inR:

    P = 1

    T T

    0 p(t)dt = 1

    R 1

    T T

    0 v2

    (t)dt =v2

    Rv2

    is the value ofv2(t)averaged over time

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)

    v(t)

    VRMS

    50 100 150 200 2500

    0.5

    1

    t (s)

    2 v2(t)

    mean(v2)

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

    Average Powerdissipated inR:

    P = 1

    T T

    0 p(t)dt = 1

    R 1

    T T

    0 v2

    (t)dt =v2

    Rv2

    is the value ofv2(t)averaged over time

    We define theRMS Voltage(Root Mean Square): Vrms =v2

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)

    v(t)

    VRMS

    50 100 150 200 2500

    0.5

    1

    t (s)

    2 v2(t)

    mean(v2)

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

    Average Powerdissipated inR:

    P = 1

    T T

    0 p(t)dt = 1

    R 1

    T T

    0 v2

    (t)dt =v2

    Rv2

    is the value ofv2(t)averaged over time

    We define theRMS Voltage(Root Mean Square): Vrms =v2

    The average power dissipated inR isP =v2

    R = (Vrms)

    2

    R

    Vrms is the DC voltage that would causeR to dissipate the same power.

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    Average Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 2 / 11

    50 100 150 200 250-1

    0

    1

    t (s)

    v(t)

    VRMS

    50 100 150 200 2500

    0.5

    1

    t (s)

    2 v2(t)

    mean(v2)

    Intantaneous Powerdissipated in R: p(t) = v2(t)R

    Average Powerdissipated inR:

    P = 1

    T T

    0 p(t)dt = 1

    R 1

    T T

    0 v2

    (t)dt =v2

    Rv2

    is the value ofv2(t)averaged over time

    We define theRMS Voltage(Root Mean Square): Vrms =v2

    The average power dissipated inR isP =v2

    R = (Vrms)

    2

    R

    Vrms is the DC voltage that would causeR to dissipate the same power.

    We usesmall lettersfor time-varying voltages andcapital lettersfor

    time-invariant values.

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    Cosine Wave RMS

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 3 / 11

    0 2 4 6 8 10-5

    0

    5

    t (ms)

    Cosine Wave: v(t) = 5 cos t. Amplitude isV = 5 V.

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    Cosine Wave RMS

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 3 / 11

    0 2 4 6 8 10-5

    0

    5

    t (ms)0 2 4 6 8 10

    0

    10

    20

    t (ms)

    2

    Cosine Wave: v(t) = 5 cos t. Amplitude isV = 5 V.

    Squared Voltage: v2(t) =V2 cos2 t=V212 +

    12cos 2t

    Mean Square Voltage: v2= V22 sincecos 2t averages to zero.

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    Cosine Wave RMS

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 3 / 11

    0 2 4 6 8 10-5

    0

    5

    t (ms)0 2 4 6 8 10

    0

    10

    20

    t (ms)

    2

    2

    Cosine Wave: v(t) = 5 cos t. Amplitude isV = 5 V.

    Squared Voltage: v2(t) =V2 cos2 t=V212 +

    12cos 2t

    Mean Square Voltage: v2= V22 sincecos 2t averages to zero.

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    Cosine Wave RMS

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 3 / 11

    0 2 4 6 8 10-5

    0

    5

    t (ms)0 2 4 6 8 10

    0

    10

    20

    t (ms)

    2

    2

    Cosine Wave: v(t) = 5 cos t. Amplitude isV = 5 V.

    Squared Voltage: v2(t) =V2 cos2 t=V212 +

    12cos 2t

    Mean Square Voltage: v2= V22 sincecos 2t averages to zero.RMS Voltage: Vrms =

    v2 = 12

    V = 3.54 V

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    Cosine Wave RMS

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 3 / 11

    0 2 4 6 8 10-5

    0

    5

    t (ms)0 2 4 6 8 10

    0

    10

    20

    t (ms)

    2

    2

    Cosine Wave: v(t) = 5 cos t. Amplitude isV = 5 V.

    Squared Voltage: v2(t) =V2 cos2 t=V212 +

    12cos 2t

    Mean Square Voltage: v2= V22 sincecos 2t averages to zero.RMS Voltage: Vrms =

    v2 = 12

    V = 3.54 V

    Note:Power engineersalwaysuse RMS voltages and currents exclusively

    and omit the rms subscript.

    For example UK Mains voltage = 230 V rms = 325 V peak.

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    Cosine Wave RMS

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 3 / 11

    0 2 4 6 8 10-5

    0

    5

    t (ms)0 2 4 6 8 10

    0

    10

    20

    t (ms)

    2

    2

    Cosine Wave: v(t) = 5 cos t. Amplitude isV = 5 V.

    Squared Voltage: v2(t) =V2 cos2 t=V212 +

    12cos 2t

    Mean Square Voltage: v2= V22 sincecos 2t averages to zero.RMS Voltage: Vrms =

    v2 = 12

    V = 3.54 V =VNote:Power engineersalwaysuse RMS voltages and currents exclusively

    and omit the rms subscript.

    For example UK Mains voltage = 230 V rms = 325 V peak.

    In this lecture course only, a ~ overbar means

    2: thus

    V = 1

    2V.

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

    Power dissipated in loadZ isp(t) =v(t)i(t) = |V| |I| cos(t + V) cos (t + I)

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

    Power dissipated in loadZ isp(t) =v(t)i(t) = |V| |I| cos(t + V) cos (t + I)

    = |V| |I| 12cos(2t + V + I) + 12cos (V I)

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

    Power dissipated in loadZ isp(t) =v(t)i(t) = |V| |I| cos(t + V) cos (t + I)

    = |V| |I| 12cos(2t + V + I) + 12cos (V I)= 12

    |V

    | |I

    |cos(V

    I) +

    12

    |V

    | |I

    |cos (2t + V + I)

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    0 2 4 6 8 10

    0

    0.5

    1

    1.5

    t (ms)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

    Power dissipated in loadZ isp(t) =v(t)i(t) = |V| |I| cos(t + V) cos (t + I)

    = |V| |I| 12cos(2t + V + I) + 12cos (V I)= 12

    |V

    | |I

    |cos(V

    I) +

    12

    |V

    | |I

    |cos (2t + V + I)

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    0 2 4 6 8 10

    0

    0.5

    1

    1.5

    t (ms)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

    Power dissipated in loadZ isp(t) =v(t)i(t) = |V| |I| cos(t + V) cos (t + I)

    = |V| |I| 12cos(2t + V + I) + 12cos (V I)= 12

    |V

    | |I

    |cos(V

    I) +

    12

    |V

    | |I

    |cos (2t + V + I)

    Average power: P = 12 |V| |I| cos() where =V I

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    0 2 4 6 8 10

    0

    0.5

    1

    1.5

    t (ms)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

    Power dissipated in loadZ isp(t) =v(t)i(t) = |V| |I| cos(t + V) cos (t + I)

    = |V| |I| 12cos(2t + V + I) + 12cos (V I)= 12

    |V

    | |I

    |cos(V

    I) +

    12

    |V

    | |I

    |cos (2t + V + I)

    Average power: P = 12 |V| |I| cos() where =V I=V I cos() cos is thepower factor

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    Power Factor

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 4 / 11

    0 2 4 6 8 10-2

    0

    2

    t (ms)

    v(t)i(t)

    0 2 4 6 8 10

    0

    0.5

    1

    1.5

    t (ms)

    Suppose voltage and current phasors are:

    V = |V| ejV v(t) = |V| cos(t + V)I= |I| ejI i(t) = |I| cos(t + I)

    Power dissipated in loadZ isp(t) =v(t)i(t) = |V| |I| cos(t + V) cos (t + I)

    = |V| |I| 12cos(2t + V + I) + 12cos (V I)= 12

    |V

    | |I

    |cos(V

    I) +

    12

    |V

    | |I

    |cos (2t + V + I)

    Average power: P = 12 |V| |I| cos() where =V I=V I cos() cos is thepower factor

    >0 alagging power factor(normal case: Current lags Voltage)

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQ

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQ

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQComplex Power: S=VI =P+jQmeasured inVolt-Amps(VA)

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQComplex Power: S=VI =P+jQmeasured inVolt-Amps(VA)Apparent Power: |S| =

    V Imeasured inVolt-Amps(VA)

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQComplex Power: S=VI =P+jQmeasured inVolt-Amps(VA)Apparent Power: |S| =

    V Imeasured inVolt-Amps(VA)Average Power: P =

    (S)measured inWatts(W)

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQComplex Power: S=VI =P+jQmeasured inVolt-Amps(VA)Apparent Power: |S| =

    V Imeasured inVolt-Amps(VA)Average Power: P =

    (S)measured inWatts(W)

    Reactive Power: Q= (S)Measured inVolt-Amps Reactive(VAR)

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQComplex Power: S=VI =P+jQmeasured inVolt-Amps(VA)Apparent Power: |S| =

    V Imeasured inVolt-Amps(VA)Average Power: P =

    (S)measured inWatts(W)

    Reactive Power: Q= (S)Measured inVolt-Amps Reactive(VAR)Power Factor: cos = cos

    V I= P|S|

    Machines and transformers have capacity limits and power losses that are

    independent ofcos ; their ratings are always given inapparent power.

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    Complex Power

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 5 / 11

    If V = 12|V| ejV and I= 1

    2|I| ejI

    Thecomplex powerabsorbed byZ isS=VIwhere * means complex conjugate.

    VI= V ejV I ejI = V I ej(VI)=V I ej = V I cos +j V I sin

    =P+jQComplex Power: S=VI =P+jQmeasured inVolt-Amps(VA)Apparent Power: |S| =

    V Imeasured inVolt-Amps(VA)Average Power: P =

    (S)measured inWatts(W)

    Reactive Power: Q= (S)Measured inVolt-Amps Reactive(VAR)Power Factor: cos = cos

    V I= P|S|

    Machines and transformers have capacity limits and power losses that are

    independent ofcos ; their ratings are always given inapparent power.Power Company:Costs apparent power, Revenue average power.

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    Power in R, L, C

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 6 / 11

    For any impedance,Z, complex power absorbed: S=VI =P+jQ

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    Power in R, L, C

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 6 / 11

    For any impedance,Z, complex power absorbed: S=VI =P+jQUsing (a)V =IZ (b)II = I2 we getS= I2 Z=|V|2Z

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    Power in R, L, C

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 6 / 11

    For any impedance,Z, complex power absorbed: S=VI =P+jQUsing (a)V =IZ (b)II = I2 we getS= I2 Z=|V|2Z

    Resistor: S= I2

    R=|V

    |2

    R = 0

    Absorbs average power,no VARs(Q= 0)

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    Power in R, L, C

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 6 / 11

    For any impedance,Z, complex power absorbed: S=VI =P+jQUsing (a)V =IZ (b)II = I2 we getS= I2 Z=|V|2Z

    Resistor: S= I2

    R=|V

    |2

    R = 0

    Absorbs average power,no VARs(Q= 0)

    Inductor: S=j I2

    L =j |V

    |2

    L = +90

    No average power,Absorbs VARs(Q >0)

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    Power in R, L, C

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 6 / 11

    For any impedance,Z, complex power absorbed: S=VI =P+jQUsing (a)V =IZ (b)II = I2 we getS= I2 Z=|V|2Z

    Resistor: S= I2

    R=|V

    |2

    R = 0

    Absorbs average power,no VARs(Q= 0)

    Inductor: S=j I2

    L =j |V

    |2

    L = +90

    No average power,Absorbs VARs(Q >0)

    Capacitor:S= j |I

    |2

    C = j V2

    C = 90No average power,Generates VARs(Q

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    Power in R, L, C

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 6 / 11

    For any impedance,Z, complex power absorbed: S=VI =P+jQUsing (a)V =IZ (b)II = I2 we getS= I2 Z=|V|2Z

    Resistor: S= I2

    R=|V

    |2

    R = 0

    Absorbs average power,no VARs(Q= 0)

    Inductor: S=j I2

    L =j |V

    |2

    L = +90

    No average power,Absorbs VARs(Q >0)

    Capacitor:S= j |I

    |2

    C = j V2

    C = 90No average power,Generates VARs(Q

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    Power in R, L, C

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 6 / 11

    For any impedance,Z, complex power absorbed: S=VI =P+jQUsing (a)V =IZ (b)II = I2 we getS= I2 Z=|V|2Z

    Resistor: S= I2

    R=|V

    |2

    R = 0

    Absorbs average power,no VARs(Q= 0)

    Inductor: S=j I2

    L =j |V

    |2

    L = +90

    No average power,Absorbs VARs(Q >0)

    Capacitor:S= j |I

    |2

    C = j V2

    C = 90No average power,Generates VARs(Q

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    Tellegens Theorem

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 7 / 11

    Tellegens Theorem:The complex power,S, dissipated in any circuitscomponents sums to zero.

    xn=voltage at nodenVb, Ib=voltage/current in branchb

    (obeying passive sign convention)

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    Tellegens Theorem

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 7 / 11

    Tellegens Theorem:The complex power,S, dissipated in any circuitscomponents sums to zero.

    xn=voltage at nodenVb, Ib=voltage/current in branchb

    (obeying passive sign convention)

    abn=

    1 ifVb starts from noden+1 ifVb ends at noden

    0 else

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    Tellegens Theorem

    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 7 / 11

    Tellegens Theorem:The complex power,S, dissipated in any circuitscomponents sums to zero.

    xn=voltage at nodenVb, Ib=voltage/current in branchb

    (obeying passive sign convention)

    abn=

    1 ifVb starts from noden+1 ifVb ends at noden

    0 elsee.g. branch 4 goes from 2 to 3 a4= [0,1, 1]

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    Tellegens Theorem

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 7 / 11

    Tellegens Theorem:The complex power,S, dissipated in any circuitscomponents sums to zero.

    xn=voltage at nodenVb, Ib=voltage/current in branchb

    (obeying passive sign convention)

    abn=

    1 ifVb starts from noden+1 ifVb ends at noden

    0 elsee.g. branch 4 goes from 2 to 3 a4= [0,1, 1]

    Branch voltages: Vb =

    n abnxn (e.g. V4 =x3 x2)

    KCL @ noden: b abnIb = 0 b abnIb = 0

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    Tellegens Theorem

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 7 / 11

    Tellegens Theorem:The complex power,S, dissipated in any circuitscomponents sums to zero.

    xn=voltage at nodenVb, Ib=voltage/current in branchb

    (obeying passive sign convention)

    abn=

    1 ifVb starts from noden+1 ifVb ends at noden

    0 elsee.g. branch 4 goes from 2 to 3 a4= [0,1, 1]

    Branch voltages: Vb =

    n abnxn (e.g. V4 =x3 x2)

    KCL @ noden: b abnIb = 0 b abnIb = 0Tellegen:

    b VbI

    b =

    b

    n abnxnI

    b

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    Tellegens Theorem

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 7 / 11

    Tellegens Theorem:The complex power,S, dissipated in any circuitscomponents sums to zero.

    xn=voltage at nodenVb, Ib=voltage/current in branchb

    (obeying passive sign convention)

    abn=

    1 ifVb starts from noden+1 ifVb ends at noden

    0 elsee.g. branch 4 goes from 2 to 3 a4= [0,1, 1]

    Branch voltages: Vb =

    n abnxn (e.g. V4 =x3 x2)

    KCL @ noden: b abnIb = 0 b abnIb = 0Tellegen:

    b VbI

    b =

    b

    n abnxnI

    b

    =

    n

    b abnI

    b xn

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    Tellegens Theorem

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 7 / 11

    Tellegens Theorem:The complex power,S, dissipated in any circuitscomponents sums to zero.

    xn=voltage at nodenVb, Ib=voltage/current in branchb

    (obeying passive sign convention)

    abn=

    1 ifVb starts from noden+1 ifVb ends at noden

    0 elsee.g. branch 4 goes from 2 to 3 a4= [0,1, 1]

    Branch voltages: Vb =

    n abnxn (e.g. V4 =x3 x2)

    KCL @ noden: b abnIb = 0 b abnIb = 0Tellegen:

    b VbI

    b =

    b

    n abnxnI

    b

    =

    n

    b abnI

    b xn=

    n xn

    b abnI

    b =

    n xn 0

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A

    P F C i

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36

    P F C i

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA

    P F t C ti

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVA

    P F t C ti

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVAcos = P

    |S|= cos 36 = 0.81

    P F t C ti

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVAcos = P

    |S|= cos 36 = 0.81

    Add parallel capacitor of300 F:

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    Power Factor Correction

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVAcos = P

    |S|= cos 36 = 0.81

    Add parallel capacitor of300 F:ZC=

    1jC

    = 10.6j IC= 21.7j A

    Power Factor Correction

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVAcos = P

    |S|= cos 36 = 0.81

    Add parallel capacitor of300 F:ZC=

    1jC

    = 10.6j IC= 21.7j AI= 46

    j11.2 A= 47

    14A

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    Power Factor Correction

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVAcos = P

    |S|= cos 36 = 0.81

    Add parallel capacitor of300 F:ZC=

    1jC

    = 10.6j IC= 21.7j AI= 46

    j11.2 A= 47

    14A

    SC=VIC= j5 kVAS=VI = 10.6 + j2.6 kVA

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    Power Factor Correction

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVAcos = P

    |S|= cos 36 = 0.81

    Add parallel capacitor of300 F:ZC=

    1jC

    = 10.6j IC= 21.7j AI= 46

    j11.2 A= 47

    14A

    SC=VIC= j5 kVAS=VI = 10.6 + j2.6 kVA = 10.914kVAcos = P

    |S

    |= cos 14 = 0.97

    Average power to motor,P, is10.6 kW in both cases.

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    Power Factor Correction

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    Power Factor Correction

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 8 / 11

    V= 230. Motor modelled as5||7j .I= VR

    + VZL

    = 46j32.9 A = 56.5 36S=VI = 10.6 + j7.6 kVA = 1336kVAcos = P

    |S|= cos 36 = 0.81

    Add parallel capacitor of300 F:ZC=

    1jC

    = 10.6j IC= 21.7j AI= 46

    j11.2 A= 47

    14A

    SC=VIC= j5 kVAS=VI = 10.6 + j2.6 kVA = 10.914kVAcos = P

    |S

    |= cos 14 = 0.97

    Average power to motor,P, is10.6 kW in both cases.I

    , reduced from56.5 47 A (16%) lower losses.Effect ofC: VARs= 7.6 2.6 kVAR , power factor= 0.81 0.97.

    Ideal Transformer

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    Ideal Transformer

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ideal Transformer

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    Ideal Transformer

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ampres law:

    NrIr = lA

    ;Faradays law: VrNr

    = ddt

    .

    Ideal Transformer

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    Ideal Transformer

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ampres law:

    NrIr = lA

    ;Faradays law: VrNr

    = ddt

    .

    N1 :N2+ N3 shows the turns ratio between the windings.

    The indicates the voltage polarity of each winding.

    Ideal Transformer

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    Ideal Transformer

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ampres law:

    NrIr = lA

    ;Faradays law: VrNr

    = ddt

    .

    N1 :N2+ N3 shows the turns ratio between the windings.

    The indicates the voltage polarity of each winding.Since is the same for all windings, V1

    N1= V2

    N2= V3

    N3.

    Ideal Transformer

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    dea a s o e

    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ampres law:

    NrIr = lA

    ;Faradays law: VrNr

    = ddt

    .

    N1 :N2+ N3 shows the turns ratio between the windings.

    The indicates the voltage polarity of each winding.Since is the same for all windings, V1

    N1= V2

    N2= V3

    N3.

    Assume N1I1+ N2I2+ N3I3 = 0

    Ideal Transformer

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    14: Power in AC Circuits Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ampres law:

    NrIr = lA

    ;Faradays law: VrNr

    = ddt

    .

    N1 :N2+ N3 shows the turns ratio between the windings.

    The indicates the voltage polarity of each winding.Since is the same for all windings, V1

    N1= V2

    N2= V3

    N3.

    Assume N1I1+ N2I2+ N3I3 = 0These two equations allow you to solve circuits and also

    imply that

    Si= 0.

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    Ideal Transformer

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ampres law:

    NrIr = lA

    ;Faradays law: VrNr

    = ddt

    .

    N1 :N2+ N3 shows the turns ratio between the windings.

    The indicates the voltage polarity of each winding.Since is the same for all windings, V1

    N1= V2

    N2= V3

    N3.

    Assume N1I1+ N2I2+ N3I3 = 0These two equations allow you to solve circuits and also

    imply that

    Si= 0.

    Special Case:

    For a 2-winding transformer this simplifies toV2 =

    N2N1

    V1 andIL = I2 = N1N2 I1

    Ideal Transformer

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 9 / 11

    A transformer has 2windings on the same magneticcore.

    Ampres law:

    NrIr = lA

    ;Faradays law: VrNr

    = ddt

    .

    N1 :N2+ N3 shows the turns ratio between the windings.

    The indicates the voltage polarity of each winding.Since is the same for all windings, V1

    N1= V2

    N2= V3

    N3.

    Assume N1I1+ N2I2+ N3I3 = 0These two equations allow you to solve circuits and also

    imply that

    Si= 0.

    Special Case:

    For a 2-winding transformer this simplifies toV2 =

    N2N1

    V1 andIL = I2 = N1N2 I1

    Hence V1I1

    =N1N2

    2V2IL

    =N1N2

    2Z

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    Transformer Applications

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 10 / 11

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    Transformer Applications

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 10 / 11

    Power Transmission

    Suppose a power transmission cable has1 resistance.100 kVA@1 kV =100 A I2R= 10 kW losses.100 kVA@100 kV =1 A

    I2R= 1 W losses.

    Transformer Applications

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 10 / 11

    Power Transmission

    Suppose a power transmission cable has1 resistance.100 kVA@1 kV =100 A I2R= 10 kW losses.100 kVA@100 kV =1 A

    I2R= 1 W losses.

    Voltage Conversion

    Electronic equipment requires 20 V but mains voltage is240 V .

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    Transformer Applications

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 10 / 11

    Power Transmission

    Suppose a power transmission cable has1 resistance.100 kVA@1 kV =100 A I2R= 10 kW losses.100 kVA@100 kV =1 A

    I2R= 1 W losses.

    Voltage Conversion

    Electronic equipment requires 20 V but mains voltage is240 V .Interference protection

    Microphone on long cable is susceptible to interference from nearby mains

    cables. AnN : 1transformer reduces the microphone voltage byN butreduces interference byN2.

    Isolation

    There is no electrical connection between the windings of a transformer so

    circuitry (or people) on one side will not be endangered by a failure that

    results in high voltages on the other side.

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    Summary

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 11 / 11

    Complex Power: S=VI =P+jQwhereV =Vrms = 12V. For an impedanceZ:S=

    I2 Z=|V|2Z

    Summary

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 11 / 11

    Complex Power: S=VI =P+jQwhereV =Vrms = 12V. For an impedanceZ:S=

    I2 Z=|V|2Z

    Apparent Power:

    |S

    |=VI

    used for machine ratings.

    Summary

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 11 / 11

    Complex Power: S=VI =P+jQwhereV =Vrms = 12V. For an impedanceZ:S=

    I2 Z=|V|2Z

    Apparent Power:

    |S

    |=VI

    used for machine ratings.

    Average Power: P = (S) = V I cos (inWatts) Reactive Power: Q= (S) =

    V I sin (inVARs)

    Summary

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 11 / 11

    Complex Power: S=VI =P+jQwhereV =Vrms = 12V. For an impedanceZ:S=

    I2 Z=|V|2Z

    Apparent Power:

    |S

    |=VI

    used for machine ratings.

    Average Power: P = (S) = V I cos (inWatts) Reactive Power: Q= (S) =

    V I sin (inVARs)

    Power engineers alwaysuseV andIand omit the ~.

    Summary

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 11 / 11

    Complex Power: S=VI =P+jQwhereV =Vrms = 12V. For an impedanceZ:S=

    I2 Z=|V|2Z

    Apparent Power:

    |S

    |=VI

    used for machine ratings.

    Average Power: P = (S) = V I cos (inWatts) Reactive Power: Q= (S) =

    V I sin (inVARs)

    Power engineers alwaysuseV andIand omit the ~. Tellegen:In any circuit b Sb= 0 b Pb =b Qb = 0

    Summary

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    E1.1 Analysis of Circuits (2014-4121) AC Power: 14 11 / 11

    Complex Power: S=VI =P+jQwhereV =Vrms = 12V. For an impedanceZ:S=

    I2 Z=|V|2Z

    Apparent Power:

    |S

    |=VI

    used for machine ratings.

    Average Power: P = (S) = V I cos (inWatts) Reactive Power: Q= (S) =

    V I sin (inVARs)

    Power engineers alwaysuse

    V and

    Iand omit the ~.

    Tellegen:In any circuit b Sb= 0 b Pb =b Qb = 0 Power Factor Correction: add parallelCto generate extra VARs

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    Summary

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    14: Power in AC Circuits

    Average Power

    Cosine Wave RMS

    Power Factor

    Complex Power

    Power in R, L, C

    Tellegens Theorem

    Power Factor Correction

    Ideal Transformer

    Transformer Applications

    Summary

    Complex Power: S=VI =P+jQwhereV =Vrms = 12V. For an impedanceZ:S=

    I2 Z=|V|2Z

    Apparent Power:

    |S

    |=VI

    used for machine ratings.

    Average Power: P = (S) = V I cos (inWatts) Reactive Power: Q= (S) =

    V I sin (inVARs)

    Power engineers alwaysuse

    V and

    Iand omit the ~.

    Tellegen:In any circuit b Sb= 0 b Pb =b Qb = 0 Power Factor Correction: add parallelCto generate extra VARs

    Ideal Transformer:Vi Ni and NiIi = 0(implies Si = 0)See Irwin & Nelms Chapter 9.