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![Page 1: Power in AC Circuits ELEC 308 Elements of Electrical Engineering Dr. Ron Hayne Images Courtesy of Allan Hambley and Prentice-Hall.](https://reader030.fdocuments.us/reader030/viewer/2022032803/56649e1b5503460f94b09a74/html5/thumbnails/1.jpg)
Power in AC Circuits
ELEC 308
Elements of Electrical Engineering
Dr. Ron Hayne
Images Courtesy of Allan Hambley and Prentice-Hall
![Page 2: Power in AC Circuits ELEC 308 Elements of Electrical Engineering Dr. Ron Hayne Images Courtesy of Allan Hambley and Prentice-Hall.](https://reader030.fdocuments.us/reader030/viewer/2022032803/56649e1b5503460f94b09a74/html5/thumbnails/2.jpg)
Power Delivered to a Load
ELEC 308 2
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RESISTIVE Load
Pure Resistance Current in Phase
with Voltage
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mm
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2cos
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![Page 4: Power in AC Circuits ELEC 308 Elements of Electrical Engineering Dr. Ron Hayne Images Courtesy of Allan Hambley and Prentice-Hall.](https://reader030.fdocuments.us/reader030/viewer/2022032803/56649e1b5503460f94b09a74/html5/thumbnails/4.jpg)
INDUCTIVE Load
Pure Inductance Current Lags Voltage Reactive power flows from
source to load; Pavg = ______
ELEC 308 4
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mm
mm
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sincos
sin90cos
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![Page 5: Power in AC Circuits ELEC 308 Elements of Electrical Engineering Dr. Ron Hayne Images Courtesy of Allan Hambley and Prentice-Hall.](https://reader030.fdocuments.us/reader030/viewer/2022032803/56649e1b5503460f94b09a74/html5/thumbnails/5.jpg)
CAPACITIVE Load
Pure Capacitance Current Leads Voltage Reactive power flows from
source to load; Pavg = ______
ELEC 308 5
ttIVtitvtp
tItIti
tVtv
CCjZ
mm
mm
m
C
sincos
sin90cos
cos
9011
![Page 6: Power in AC Circuits ELEC 308 Elements of Electrical Engineering Dr. Ron Hayne Images Courtesy of Allan Hambley and Prentice-Hall.](https://reader030.fdocuments.us/reader030/viewer/2022032803/56649e1b5503460f94b09a74/html5/thumbnails/6.jpg)
Importance of Reactive Power
No average power is consumed by a pure energy-storage element
Reactive power still important Transmission lines, transformers, fuses, etc. must be
able to withstand the current associated with reactive power
Possible to have loads that draw LARGE currents, even though little average power is consumed
Electric power companies STILL charge for reactive power (at a lower rate), as well as total energy delivered
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Real Power
ELEC 308 7
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m
m
RLCRLC
cos
cos
(W). in watts are power (REAL) average of Units
cos
cos22
cos2
P
IV
IVIVP
rmsrms
mmmm
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Power Factor
The term cos(θ) is called the power factor: PF = cos(θ)
The power angle θ is taken as the phase of the voltage θv minus the phase of the current θi
θ = θv-θi
Current lags voltage = POSITIVE power angle Current leads voltage = NEGATIVE power angle
Sometimes stated as a PERCENTAGE e.g. 90% lagging => cos(θ) = 0.9 and Curr. lags Volt.
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Reactive Power
Capacitance voltage increasing/decreasing Energy flowing into/out of capacitance
Inductance current increasing/decreasing Energy flowing into/out of inductance
Instantaneous power can be VERY large Average power (and net energy) is still _________
Reactive power is peak instantaneous power associated with energy-storage elements Q = VrmsIrmssin(θ) Units are VARs (Volt Amperes Reactive)
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Apparent Power
Apparent power is the product of the effective voltage and effect current S = VrmsIrms
Units are volt-amperes (VA) Can be determined from real and reactive
powers:
ELEC 308 10
22 QPS
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Units
Units indicate whether quantity is power, reactive power, or apparent power 5-kW load means that P = 5 kW 5-kVA load means that VrmsIrms = 5 kVA 5-kVAR load means that Q = 5 kVAR
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Power Triangle
Demonstrates relationships between Real power, P Reactive power, Q Apparent power VrmsIrms Power angle, θ
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Additional Power Relationships
X
VQ
XIQ
R
VP
RIP
rms
rms
rms
rms
2
2
2
2
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Using Power Triangles
Find the power, reactive power, and power factor for the source in the circuit below.
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Using Power Triangles
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Using Power Triangles
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Power Factor Correction
In heavy industry Many loads are partly inductive = large amounts of
reactive power flow Causes higher current in transmission system
Energy rates charged to industry depend on the power factor Higher charges for energy delivered at lower power
factors Advantageous to choose loads that operate at near
unity power factor Common approach is to place capacitors in parallel
with an inductive load to increase the power factor
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Thévenin and Norton
Use same techniques for circuits with impedances as we did for resistive circuits
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Maximum Power Transfer
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Maximum Power Transfer
Maximum power transferred achieved by maximizing the current
First case: Load is complex impedance Load impedance for max. power transfer is
Reactance of load CANCELS internal reactance of two-terminal circuit
Second case: Load is pure resistance Load impedance for max. power transfer is
ELEC 308 20
Z load Zt
Z load Rload Z t
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Maximum Power Transfer
Determine the maximum power that can be delivered to a load by the two-terminal resistance below if The load can be any complex impedance The load must be a pure resistance
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Summary
AC Power Real Power Reactive Power Apparent Power Power Factor
Thevenin and Norton Maximum Power Transfer
ELEC 308 22