01400_acpower.pdf
TRANSCRIPT
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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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-
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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.