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Linear Circuits at ac
Instantaneous power Average power
)()()( tittp
Power at any instant of time Average of instantaneous power over one period
T
dttpT
P0
)(1
Power delivery (utilities) Electronics (laptops, mobile phones, etc.) Logic circuits
Power is critical for many reasons:
Note: Power is not a linear function, cannot apply superposition
Instantaneous Power for Sinusoids
Power depends on phases of voltage and current
i
i
ttIVtp
tittp
tIti
tVt
coscos)(
)()()(
cos)(
cos)(
mm
m
m
BABABA coscos2
1coscos
ii tIVtp 2coscos2
1)( mm
Trig. Identity:
Constant in time (dc term)
ac at 2w
Effective or RMS Value
Equivalent Value That Delivers Same Average Power to Resistor as in dc case
For current given by
Effective value is the (square) Root of the Mean of the Square of the periodic signal, or RMS value
TTdti
T
RdtRi
TP
0
2
0
21
RIP 2eff
Tdti
TI
0
2eff
1 T
dtT
V0
2eff
1
tIti cosm 2
cos1 m
0
22mrms
IdttI
TI
T
Hence:
Similarly,
Average Power
i
i
ttIVtp
tittp
tIti
tVt
coscos)(
)()()(
cos)(
cos)(
mm
m
m
ii tIVtp 2coscos2
1)( mm
BABABA coscos2
1coscos
Note dependence on phase difference
Average Power
Since and a similar relationship applies to I,
Power factor angle:
0 for a resistor= 90 degrees for inductor ‒90 degrees for capacitor
ac Power Capacitors
2
i
dt
dCi C
C
CC CVjI
2CC CVI
Capacitors (ideal) dissipate zero average power
222cos2
1
2coscos2
1
mm
mm
tIVtp
tIVtp ii
= 0
ac Power Inductors
2
i
dt
diL L
L
LL LIjV
2LL iLIV
Inductors (ideal) dissipate zero average power
222cos2
1
2coscos2
1
mm
mm
i
ii
tIVtp
tIVtp
= 0
Power Factor for Complex LoadInductive/capacitive loads will require more from the power supply than the average power being consumed Power supply needs to
supply S in order to deliver Pav to load
Power factor relates S to Pav
Maximum Power Transfer
Max power is delivered to load if load is equal to Thévenin equivalent
*sssLLL ZjXRjXRZ Max power
transfer when
Set derivatives equal to zero 0L
X
P0
L
R
P
s
2
Thmax 8R
VP