See online explanation at AC Circuits.
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Transcript of See online explanation at AC Circuits.
![Page 1: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/1.jpg)
See online explanation at
http://www.physclips.unsw.edu.au/jw/AC.html
AC Circuits
![Page 2: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/2.jpg)
Total Energy• Total energy of the system
is the sum of the electric and magnetic field energy.
tC
QU mC 2
2
cos2
tLIU mL 2
2
sin2
CL
I
B
CL+ + + +
E
22
22mm
LC
LI
C
QUUU
![Page 3: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/3.jpg)
RLC Circuit• After the switch is closed
Kirchoff’s rules gives
• Solution:
• Critical Damping:
CLI + + + +
+
R
02
2
C
Q
dt
dQR
dt
QdL
teQQ dLRt
m cos2/
2/12
2
1
L
R
LCd
C
LRc
4
![Page 4: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/4.jpg)
AC Source• The voltage of the power
supply follows that of a cosine function.
• Represent the source as a vector rotating in the complex plane.
• Real component of vector is the instantaneous voltage.
tVtv m cos)(
Im
Rev
Vm
t
Vm
-Vm
t
v
![Page 5: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/5.jpg)
AC & Resistors
• Voltage and current are in phase, = 0.
v R
tR
Vti m cos)( tVtv m cos)(
vi
Im
Rev
Vm
ti
0 Riv
FromKirchoff
![Page 6: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/6.jpg)
Power• Power used by a resistor is
• Average power is
• Effective voltage and current are
tR
VivtP m 2
2
cos)(
22
2mmm IV
R
VP
2m
rms
VV rmsrms IVP
2m
rms
II
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AC & Inductors
• Voltage leads current by 90°, = /2.
2cos)(
tL
Vti m tVtv m cos)( Im
Rev
Vm
ti
v L
v
i
0dt
diLv
FromKirchoff
LX L Reactance
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AC & Capacitors
• Voltage lags current by 90°, = -/2.
2cos)( tCVti m tVtv m cos)( Im
Rev
Vm
ti
v C
01
dtiC
v
FromKirchoff
CXC
1
Reactance
v
i
![Page 9: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/9.jpg)
LRC Circuits & AC
C
L
R
v
CLR jvjvvv Re
Im
vL
vC vR
i
• In a series circuit current is the same everywhere, so add voltages as phasors.
• Phasors are rotating vectors in the complex plane.
• Assume we are at t = 0s.
![Page 10: See online explanation at AC Circuits.](https://reader036.fdocuments.us/reader036/viewer/2022062519/5697bfc41a28abf838ca5c22/html5/thumbnails/10.jpg)
Impedance
Re
Im
vSvL
vC
vR
22CL XXRZ
iZXXjRiv CL
R
XX CL1tan
CL iXjiXjiRv
• Express voltage as current times impedance.
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ELI the ICE man• At resonance, 0, XL=XC and = 0.
• For <0, the circuit is capacitive and current leads voltage. Also < 0.
• For >0, the circuit is inductive and voltage leads current. Also > 0.
R
XX CL1tanLC
10
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Quality Factor• As the AC frequency approaches resonance,
0, the current increases.
• Quality factor indicates how sharp the current peak is around resonance.
0
Im
Low Q
High Q
R
LQ 0
0
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Transformers• A transformer consists of two
sets of coils which share the same magnetic flux.
• AC current through the primary generates a changing magnetic flux, which generates a changing voltage on the secondary.
RLv
Primary SecondaryP
P
SS V
N
NV
PPSS IVIV
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Power Lines• Ex. How much power is lost if 120V is
delivered through a 10 transmission line to a 10 load?
Compare that to transmission at 12,000 V and then stepped down to 120V at the load.
RL120V12,000V
RT
RL120V
RT
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PowerTransmission
Long Distance:230 kV
To Home:240 V
Through Town:20 kV
Less resistive lossat low current.