# 9 AC circuit power analysis

```Electric Circuits II
AC Circuit Power Analysis
Dr. Firas Obeidat
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• Conservation of AC power
• Power Triangle
• Power Factor Correction
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Dr. Firas Obeidat – Philadelphia University
Conservation of AC Power
The complex, real, and reactive powers of the sources equal the respective sums
of the complex, real, and reactive powers of the individual loads.
The principle of conservation of power applies to ac circuits can be explained
by considering AC parallel circuit and AC series circuit.
ο AC parallel circuit
two load impedances Z1 and Z2 are connected in
parallel across an ac source V. KCL gives
ππ«π¦π¬ = πππ«π¦π¬ +πππ«π¦π¬
The complex power supplied by the source is
π = ππ«π¦π¬ ππ«π¦π¬ ∗ = ππ«π¦π¬ (πππ«π¦π¬ ∗ +πππ«π¦π¬ ∗ ) = ππ«π¦π¬ πππ«π¦π¬ ∗ +ππ«π¦π¬ πππ«π¦π¬ ∗ = ππ + ππ
Where S1 and S2 denote the complex powers delivered to loads Z1 and Z2.
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Dr. Firas Obeidat – Philadelphia University
Conservation of AC Power
ο AC series circuit
If the loads are connected in series with the voltage
source, KVL yields
ππ«π¦π¬ = πππ«π¦π¬ +πππ«π¦π¬
The complex power supplied by the source is
π = ππ«π¦π¬ ππ«π¦π¬ ∗ = (πππ«π¦π¬ +πππ«π¦π¬ )ππ«π¦π¬ ∗ = πππ«π¦π¬ ππ«π¦π¬ ∗ +πππ«π¦π¬ ππ«π¦π¬ ∗ = ππ + ππ
Where S1 and S2 denote the complex powers delivered to loads Z1 and Z2.
From the above discussion, it can be concluded that whether the loads are
connected in series or in parallel (or in general), the total power supplied by the
source equals the total power delivered to the load. Thus, in general, for a source
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
The three quantities average power, apparent power, and reactive power can be
related in the vector domain by
π = ππ«π¦π¬ ππ«π¦π¬ ∗ =P+jQ
π°π‘ππ«π
π = π∠0,
ππ = πππΏ = ππΏ ∠90,
ππ = −πππΆ = ππΆ ∠ − 90
For an inductive load, the phasor power S is
π=P+jπΈπ³
As in figure (a)
For an capacitive load, the phasor power S is
π=P-jπΈπͺ
As in figure (b)
When solving problems involving power, P
values can be added to get PT, and Q values
to get QT (where Q is positive for inductive
elements and negative for capacitive).
(a)
(b)
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
Example: The P and Q values for a circuit are shown
in the figure.
a. Determine the power triangle.
b. Determine the rms current supplied by the source.
(a)
PT = 700 + 800 + 80 + 120 = 1700 W
Q T = 1300 − 600 − 100 − 1200
Q T = −600 VAR
ST = PT +jQ T =1700-j600=1803∠-19.4o
(b) πΌπππ  =
π
ππππ
1803 VA
=
= 15 π΄πππ
120 V
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
Example: The circuit shows a load being fed by a voltage source through a
transmission line. The impedance of the line is represented by (4+j2)Ω the impedance
and a return path. Find the real power and reactive power absorbed by: (a) the source,
(b) the line, and (c) the load.
(a) For the source
ππ¬ = ππ¬π«π¦π¬ ππ«π¦π¬ ∗
The real power is 2163.5 W and the reactive power is 910.8 VAR (leading).
(b) For the line
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
ππ₯π’π§π = ππ₯π’π§ππ«π¦π¬ ππ«π¦π¬ ∗
The real power is 455.4 W and the reactive power is
227.76 VAR (lagging).
ππ = πππ«π¦π¬ ππ«π¦π¬ ∗
The real power is 1708 W and the
reactive power is 1139 VAR (leading).
Note that SS=Sline+SL
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
Example: A generator (its voltage in rms) supplies power to an electric heater, an
inductive element, and a capacitor as in the figure.
a. Find P and Q for each load.
b. Find total active and reactive power supplied by the generator.
c. Draw the power triangle for the combined loads and determine total apparent
power.
d. Find the current supplied by the generator.
(a) The components of power are as follows:
(b)
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
(c)
The apparent power is 3081VA
(c) Generator current is
πΌ=
ππ 3081VA
=
= 25.7 π΄πππ
π
120 V
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
Example: In the circuit, Z1=60∠-30oΩ and Z2=40∠45oΩ. Calculate the total: (a)
apparent power, (b) real power, (c) reactive power, and (d) pf, supplied by the source
and seen by the source.
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
Example: For the circuit, calculate the complex power for each load then draw the
power triangle.
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
Example: for the circuit find (the values are given in rms)
a. Find the average power, apparent power, reactive power, and pf for each branch.
b. Find the total number of watts, volt-amperes reactive, volt-amperes, and the power
factor of the system. Sketch the power triangle.
(a) βΊ Bulbs
βΊ Heating elements
π1 = 12 &times; 60W = 720W
π2 = 6.4 kW
π1 = 0 VAR
π2 = 0 VAR
π1 = π1 = 720 VA
π2 = π2 = 6.4 kVA
ππ1 = 1
ππ2 = 1
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
βΊ The motor
η=
ππ
ππ 5 &times; 746 W
→ ππ = =
= 4548.78 W
ππ
η
0.82
π3 = ππ = 4548.78W
ππ3 = 0.72 πππππππ
π3 = π3 πππ θ → π3 =
π3
4548.78 W
=
= 6317.75 VA
πππ θ
0.72
π = πππ  −1 0.72 = 43.95π
π3 = π3 π ππθ = 6317.75 &times; π ππ43.95π = 6317.75 &times; 0.694 = 4384.71 VAR (L)
Irms =
Vrms 208∠0
208∠0
=
=
= 13.87∠53.13
Z
9 − j12 15∠ − 53.13
π4 = πΌπππ  2 π = 13.872 &times; 9 = 1731.39 W
π4 = πΌπππ  2 ππΆ = 13.872 &times; 12 = 2308.52 VAR (C)
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Dr. Firas Obeidat – Philadelphia University
Power Triangle
(b)
π4 =
π4 2 + π4 2 =
ππ4 =
π4
1731.39 W
=
= 0.6 πππππππ
π4 2885.65 VA
1731.392 + 23.8.522 = 2885.65 VA
ππ = π1 +π2 +π3 +π4
ππ = 720 + 6400 + 4548.78 + 1731.39
ππ = 13400.17 W
ππ = π1 +π2 +π3 +π4
ππ = 0 + 0 + 4384.71 − 2308.52
ππ = 2076.19 VAR (πΏ)
ππ =
ππ 2 + ππ 2 =
13400.172 + 2076.192
ππ = 13560.06 VA
πππ =
ππ
13400.17 W
=
= 0.988 πππππππ
ππ 13560.06 VA
π = πππ  −1 0.988 = 8.89π
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Dr. Firas Obeidat – Philadelphia University
Power Triangle for Transformers
A transformer is a magnetically coupled circuit,
that is, a circuit in which the magnetic field
produced by time-varying current in one circuit
induces voltage in another.
Where
n : is the turns ratio or transformer ratio.
V1: is the voltage across the primary winding.
V2: is the voltage across the secondary winding.
N1: is the number of turns in the primary.
N2: is the number of turns in the secondary.
When n=1, the transformer is an isolation transformer. If
n&gt;1, the transformer is step-up transformer, as the voltage is
increased from primary to secondary (V2&gt;V1). If n&lt;1, the
transformer is step-down transformer, since the voltage is
decreased from primary to secondary (V2&lt;V1).
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Dr. Firas Obeidat – Philadelphia University
Power Triangle for Transformers
Example: A 25 kVA transformer feeds a load with 12 kW. If the pf=0.6 lagging.
transformer.
(2.a) If a unity pf load is added to the same transformer, find the power which can be
apparent power which can be added so the transformer becomes fully loaded.
(1)
Transformer apparent power is
ππ‘ππππ . = 25πVA
πππππ1 =
πππππ1 12 πW
=
= 20 πVA
ππ1
0.6
πππππ
20 πVA
%πππππππ =
&times; 100% =
&times; 100% = 80%
ππ‘ππππ .
25 πVA
π1 = πππ  −1 0.6 = 53.1π
πππππ1 = πππππ1 π ππθ = 20000 &times; π ππ53.1π = 16 kVAR
πππππ2 = 0
Pf2 =cosπ2 =1
Dr. Firas Obeidat – Philadelphia University
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Power Triangle for Transformers
πππππ = πππππ1 + πππππ2 = πππππ1 + ππππππ1 + πππππ2 + ππππππ2
πππππ = (πππππ1 + πππππ2 ) + π(πππππ1 + πππππ2 )
Before the transformer becomes fully loaded means that total load complex power equal
to transformer complex power
0
ππ‘ππππ . = πππππ = (πππππ1 + πππππ2 ) + π(πππππ1 + πππππ2 )
ππ‘ππππ . = πππππ = πππππ + ππππππ
ππ‘ππππ . 2 = πππππ 2 + πππππ 2 = (πππππ1 + πππππ2 )2 +(πππππ1 )2
252 = (12 + πππππ2 )2 +(16)2
625 − 256 = 144 + 24πππππ2 +πππππ2 2
πππππ2 2 + 24πππππ2 − 225 = 0
πππππ2 = 7.2 kW ππ − 31.21 kW
Taking the positve value
Dr. Firas Obeidat – Philadelphia University
∴ πππππ2 = 7.2 kW
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Power Triangle for Transformers
(2.b)
Pf2 =cosπ2 =0.866
π2 = πππ  −1 0.866 = 30π
πππππ2 = πππππ2 πππ 30 = 0.866πππππ2
πππππ2 = πππππ2 π ππ30 = 0.5πππππ2
πππππ = πππππ1 + πππππ2 = 12 + 0.866πππππ2
πππππ = πππππ1 − πππππ2 = 16 − 0.5πππππ2
πππππ = (πππππ1 + πππππ2 ) + π(πππππ1 + πππππ2 )
πππππ = (12 + 0.866πππππ2 ) + π(16 − 0.5πππππ2 )
Sππππ 2 = πππππ 2 + πππππ 2
252 = (12 + 0.866πππππ2 )2 +(16 − 0.5πππππ2 )2
πππππ2 = 12.8 kVA
πππππ2 = 0.866πππππ2 0.866 &times; 12.8 = 11 ππ
πππππ2 = 0.5πππππ2 = 0.5 &times; 12.8 = 6.4 kVA
Dr. Firas Obeidat – Philadelphia University
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Power Factor Correction
Most domestic loads (such as washing machines, air conditioners, and
refrigerators) and industrial loads (such as induction motors) are inductive and
operate at a low lagging power factor. Although the inductive nature of the load
cannot be changed, we can increase its power factor.
Power factor correction is the process of increasing the power factor without
altering the voltage or current to the original load.
improved or corrected by installing a capacitor in parallel with the load, as
shown in fig(b).
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Dr. Firas Obeidat – Philadelphia University
Power Factor Correction
Perspective (A)
The circuit in fig(a) has a power factor of cosθ1,
while the circuit in fig(b) has a power factor of cosθ2.
It is evident that adding the capacitor has caused the
phase angle between the supplied voltage and
current to reduce from θ1 to θ2, thereby increasing
the power factor.
From the magnitudes of the vectors, with the
same supplied voltage, the circuit in fig(a) draws
larger current IL than the current I drawn by the
circuit in fig(b).
Perspective (B)
If the original inductive load has apparent power
We want to increase the power factor from θ1 to θ2
without altering the real power
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Dr. Firas Obeidat – Philadelphia University
Power Factor Correction
The new reactive power is
The reduction in the reactive power is caused by the
shunt capacitor
But
The value of the required shunt capacitance C is determined as
ο If the load is capacitive, an inductor should be connected across the load for
power factor correction. The required shunt inductance L can be calculated
from
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Dr. Firas Obeidat – Philadelphia University
Power Factor Correction
Example: When connected to a 120 Vrms, 60-Hz power line, a load absorbs 4kW at a
lagging power factor of 0.8. Find the value of capacitance necessary to raise the pf to
0.95.
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Dr. Firas Obeidat – Philadelphia University
Power Factor Correction
Example: Suppose an industrial client is charged a penalty if the plant power factor
drops below 0.85. The equivalent plant loads are as in the figure. The frequency is 60
Hz.
a. Determine PT and QT.
b. Determine what value of capacitance is required to bring the power factor up to
0.85.
c. Determine generator current before and after correction.
a.
π1 = ππ = 132 πΎππ΄π
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Dr. Firas Obeidat – Philadelphia University
Power Factor Correction
b.
π2 =cos-1(0.85)=31.8o
π2 =PT tanπ2 =146tan31.8o=90.5 KVAR
ππΆ =Q1-Q2=132-90.5=41.5 KVAR
C=
QC
41.5&times;103
=
πVrms2 2π&times;60&times;6002
= 306 μF
c.
ST =196.8 KVA
I=
ST 196.8 πΎππ΄
=
π½
600 V
= 328 A
S2 =171.8 KVA
I=
ST 171.8 πΎππ΄
= 600 V
π½
= 286 A
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Dr. Firas Obeidat – Philadelphia University
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