Induction - Spring 20061 Time Varying Circuits April 10, 2006.
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Transcript of Induction - Spring 20061 Time Varying Circuits April 10, 2006.
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Induction - Spring 2006 1
Time Varying CircuitsTime Varying Circuits
April 10, 2006April 10, 2006
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Induction - Spring 2006 2
What is going on?What is going on?
There are only 7 more classes and There are only 7 more classes and the final is 3 weeks away.the final is 3 weeks away. Scotty, beam me somewhere else!Scotty, beam me somewhere else!
Exam IssuesExam Issues Look Ashamed!Look Ashamed!
Inductor CircuitsInductor Circuits Quiz FridayQuiz Friday AC Next week & Following MondayAC Next week & Following Monday
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Induction - Spring 2006 3
Second Problem
a a
h
Both Currents are going intothe page.
B
OtherWire
ah
stuff
hahh
dh
d
ha
h
r
h
rr
Sin
Sinr
ISintotal
(max)0)2(
~
~1
~)(
~
)(2
2)(2
22
22
0
B
B
BB
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Induction - Spring 2006 4
First Problem
V
8/
8)2(2
)(22
2
2
2
1
22
222222
2
2
mM
eRReM
consteRV
RqB
Vq
RBqm
Vq
mqBR
v
qBRm
m
Vqv
R
mvqvB
mvVq
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Induction - Spring 2006 5
The Last two Problems were similar to WebAssigns that were also reviewed in class.Circular Arc – Easy Biot-Savart
Moving Rod
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Induction - Spring 2006 6
Question
What about these problems was “unfair”?
Why so many blank or completely wrong pages?
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Induction - Spring 2006 7
And Now …..
From the past
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Induction - Spring 2006 8
Max Current Rate ofincrease = max emfVR=iR
~current
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Induction - Spring 2006 9
constant) (time
)1( /
R
L
eR
Ei LRt
Solve the lo
op equation.
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Induction - Spring 2006 10
We also showed that
2
0
2
0
2
1
2
1
E
B
capacitor
inductor
u
u
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Induction - Spring 2006 11
LR Circuit
i
then0,ELet
0
equationcapacitor
theas form same
0
:0 drops voltageof sum
dt
dqR
C
qE
dt
diLiRE
Steady Source
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Induction - Spring 2006 12
Time Dependent Result:
R
L
eR
Ei LRt
constant time
)1( /
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Induction - Spring 2006 13
R
L
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Induction - Spring 2006 14
At t=0, the charged capacitor is now connected to the inductor. What would you expect to happen??
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Induction - Spring 2006 15
The math …For an RLC circuit with no driving potential (AC or DC source):
2/12
2max
2
2
2
1
)cos(
:
0
0
L
R
LC
where
teQQ
Solutiondt
QdL
C
Q
dt
dQR
dt
diL
C
QiR
d
dL
Rt
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Induction - Spring 2006 16
The Graph of that LR (no emf) circuit ..
L
Rt
e 2
L
Rt
e 2
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Induction - Spring 2006 17
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Induction - Spring 2006 18
Mass on a Spring Result
Energy will swap back and forth. Add friction
Oscillation will slow down Not a perfect analogy
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Induction - Spring 2006 19
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Induction - Spring 2006 20
LC Circuit
High
Q/CLow
Low
High
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Induction - Spring 2006 21
The Math Solution (R=0):
LC
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Induction - Spring 2006 22
New Feature of Circuits with L and C
These circuits produce oscillations in the currents and voltages
Without a resistance, the oscillations would continue in an un-driven circuit.
With resistance, the current would eventually die out.
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Induction - Spring 2006 23
-1.5
-1
-0.5
0
0.5
1
1.5
0 1 2 3 4 5 6 7 8 9 10
Time
Vo
lts
Variable Emf Applied
emf
Sinusoidal
DC
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Induction - Spring 2006 24
Sinusoidal Stuff
)sin( tAemf
“Angle”
Phase Angle
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Induction - Spring 2006 25
Same Frequencywith
PHASE SHIFT
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Induction - Spring 2006 26
Different Frequencies
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Induction - Spring 2006 27
Note – Power is delivered to our homes as an oscillating source (AC)
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Induction - Spring 2006 28
Producing AC Generator
x x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x xx x x x x x x x x x x x x x x x x x x x x x x
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Induction - Spring 2006 29
The Real World
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Induction - Spring 2006 30
A
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Induction - Spring 2006 31
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Induction - Spring 2006 32
The Flux:
tAR
emfi
tBAemf
t
BA
bulb
sin
sin
cos
AB
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Induction - Spring 2006 33
April 12, 2006April 12, 2006
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Induction - Spring 2006 34
ScheduleSchedule
TodayToday Finish InductorsFinish Inductors
FridayFriday Quiz on this weeks materialQuiz on this weeks material Some problems and then AC circuitsSome problems and then AC circuits
MondayMonday Last FULL week of classesLast FULL week of classes Following Monday is last day of classFollowing Monday is last day of class
FINAL IS LOOMING!FINAL IS LOOMING!
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Induction - Spring 2006 35
Some ProblemsSome Problems
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Induction - Spring 2006 36
14. Calculate the resistance in an RL circuit in which L = 2.50 H and the current increases to 90.0% of its final value in 3.00 s.
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Induction - Spring 2006 37
16. Show that I = I0 e – t/τ is a solution of the differential equation where τ = L/R and I0 is the current at t = 0.
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Induction - Spring 2006 38
17. Consider the circuit in Figure P32.17, taking ε = 6.00 V, L = 8.00 mH, and R = 4.00 Ω. (a) What is the inductive time constant of the circuit? (b) Calculate the current in the circuit 250 μs after the switch is closed. (c) What is the value of the final steady-state current? (d) How long does it take the current to reach 80.0% of its maximum value?
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Induction - Spring 2006 39
18. In the circuit shown in Figure P32.17, let L = 7.00 H, R = 9.00 Ω, and ε = 120 V. What is the self-induced emf 0.200 s after the switch is closed?
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Induction - Spring 2006 40
27. A 140-mH inductor and a 4.90-Ω resistor are connected with a switch to a 6.00-V battery as shown in Figure P32.27. (a) If the switch is thrown to the left (connecting the battery), how much time elapses before the current reaches 220 mA? (b) What is the current in the inductor 10.0 s after the switch is closed? (c) Now the switch is quickly thrown from a to b. How much time elapses before the current falls to 160 mA?
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Induction - Spring 2006 41
32. At t = 0, an emf of 500 V is applied to a coil that has an inductance of 0.800 H and a resistance of 30.0 Ω. (a) Find the energy stored in the magnetic field when the current reaches half its maximum value. (b) After the emf is connected, how long does it take the current to reach this value?
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Induction - Spring 2006 42
52. The switch in Figure P32.52 is connected to point a for a long time. After the switch is thrown to point b, what are (a) the frequency of oscillation of the LC circuit, (b) the maximum charge that appears on the capacitor, (c) the maximum current in the inductor, and (d) the total energy the circuit possesses at t = 3.00 s?
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Induction - Spring 2006 43
Back to Variable Back to Variable SourcesSources
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Induction - Spring 2006 44
Source Voltage:
)sin(0 tVVemf
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Induction - Spring 2006 45
Average value of anything:
Area under the curve = area under in the average box
T
T
dttfT
h
dttfTh
0
0
)(1
)(
T
h
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Induction - Spring 2006 46
Average Value
T
dttVT
V0
)(1
0sin1
0
0 T
dttVT
V
For AC:
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Induction - Spring 2006 47
So …
Average value of current will be zero. Power is proportional to i2R and is ONLY
dissipated in the resistor, The average value of i2 is NOT zero because
it is always POSITIVE
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Induction - Spring 2006 48
Average Value
0)(1
0
T
dttVT
V
2VVrms
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Induction - Spring 2006 49
RMS
2
2)(
2
2)
2(
2
1
)2
(1
0
02
0
20
0
20
0
20
220
VV
VdSin
VV
tT
dtT
SinT
TVV
dttT
SinT
VtSinVV
rms
rms
T
rms
T
rms
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Induction - Spring 2006 50
Usually Written as:
2
2
rmspeak
peakrms
VV
VV
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Induction - Spring 2006 51
Example: What Is the RMS AVERAGE of the power delivered to the resistor in the circuit:
E
R
~
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Induction - Spring 2006 52
Power
tR
VRt
R
VRitP
tR
V
R
Vi
tVV
22
0
2
02
0
0
sin)sin()(
)sin(
)sin(
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Induction - Spring 2006 53
More Power - Details
R
VVV
RR
VP
R
VdSin
R
VP
tdtSinR
VP
dttSinTR
VP
tSinR
VtSin
R
VP
rms
T
T
200
20
20
2
0
22
0
0
22
0
0
22
0
22
022
0
22
1
2
1
2
1)(
2
1
)(1
2
)(1
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Induction - Spring 2006 54
AC CircuitsAC Circuits
April 17, 2006April 17, 2006
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Induction - Spring 2006 55
Last Days …Last Days …
If you need to, file your taxes TODAY!If you need to, file your taxes TODAY! Due at midnight.Due at midnight.
Note: File on Web has been updated.Note: File on Web has been updated. This weekThis week
Monday & Wednesday – AC Circuits Monday & Wednesday – AC Circuits followed by problem based reviewfollowed by problem based review
Friday – Review problems Next Week Friday – Review problems Next Week Monday – Complete Problem review.Monday – Complete Problem review.
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Induction - Spring 2006 56
Final ExaminationFinal Examination
Will contain 8-10 problems. One will Will contain 8-10 problems. One will probably be a collection of multiple choice probably be a collection of multiple choice questions.questions.
Problems will be Problems will be similarsimilar to WebAssign to WebAssign problems. Class problems may also be a problems. Class problems may also be a source.source.
You have 3 hours for the examination.You have 3 hours for the examination. SCHEDULE: MONDAY, MAY 1 @ 10:00 AMSCHEDULE: MONDAY, MAY 1 @ 10:00 AM
http://pegasus.cc.ucf.edu/%7Eenrsvc/registrar/http://pegasus.cc.ucf.edu/%7Eenrsvc/registrar/calendar/exam/calendar/exam/
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Induction - Spring 2006 57
Back to ACBack to AC
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Induction - Spring 2006 58
Resistive Circuit
We apply an AC voltage to the circuit. Ohm’s Law Applies
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Induction - Spring 2006 59
Con
sid
er
this
cir
cuit
CURRENT ANDVOLTAGE IN PHASE
R
emfi
iRe
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Induction - Spring 2006 60
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Induction - Spring 2006 61
Alternating Current Circuits
is the angular frequency (angular speed) [radians per second].
Sometimes instead of we use the frequency f [cycles per second]
Frequency f [cycles per second, or Hertz (Hz)] f
V = VP sin (t -v ) I = IP sin (t -I )
An “AC” circuit is one in which the driving voltage andhence the current are sinusoidal in time.
v
V(t)
t
Vp
-Vp
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Induction - Spring 2006 62
v
V(t)
t
Vp
-Vp
V = VP sin (wt - v )Phase Term
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Induction - Spring 2006 63
Vp and Ip are the peak current and voltage. We also use the
“root-mean-square” values: Vrms = Vp / and Irms=Ip /
v and I are called phase differences (these determine whenV and I are zero). Usually we’re free to set v=0 (but not I).
2 2
Alternating Current Circuits
V = VP sin (t -v ) I = IP sin (t -I )
v
V(t)
t
Vp
-Vp
Vrms
I/
I(t)
t
Ip
-Ip
Irms
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Induction - Spring 2006 64
Example: household voltage
In the U.S., standard wiring supplies 120 V at 60 Hz. Write this in sinusoidal form, assuming V(t)=0 at t=0.
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Induction - Spring 2006 65
Example: household voltage
In the U.S., standard wiring supplies 120 V at 60 Hz. Write this in sinusoidal form, assuming V(t)=0 at t=0.
This 120 V is the RMS amplitude: so Vp=Vrms = 170 V.2
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Induction - Spring 2006 66
Example: household voltage
In the U.S., standard wiring supplies 120 V at 60 Hz. Write this in sinusoidal form, assuming V(t)=0 at t=0.
This 120 V is the RMS amplitude: so Vp=Vrms = 170 V.This 60 Hz is the frequency f: so =2f=377 s -1.
2
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Induction - Spring 2006 67
Example: household voltage
In the U.S., standard wiring supplies 120 V at 60 Hz. Write this in sinusoidal form, assuming V(t)=0 at t=0.
This 120 V is the RMS amplitude: so Vp=Vrms = 170 V.This 60 Hz is the frequency f: so =2f=377 s -1.
So V(t) = 170 sin(377t + v).Choose v=0 so that V(t)=0 at t=0: V(t) = 170 sin(377t).
2
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Induction - Spring 2006 68
Review: Resistors in AC Circuits
ER
~EMF (and also voltage across resistor): V = VP sin (t)Hence by Ohm’s law, I=V/R:
I = (VP /R) sin(t) = IP sin(t) (with IP=VP/R)
V and I“In-phase”
V
t
I
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Induction - Spring 2006 69
This looks like IP=VP/R for a resistor (except for the phase change). So we call Xc = 1/(C) the Capacitive Reactance
Capacitors in AC Circuits
E
~C Start from: q = C V [V=Vpsin(t)]
Take derivative: dq/dt = C dV/dtSo I = C dV/dt = C VP cos (t)
I = C VP sin (t + /2)
The reactance is sort of like resistance in that IP=VP/Xc. Also, the current leads the voltage by 90o (phase difference).
V
t
I
V and I “out of phase” by 90º. I leads V by 90º.
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Induction - Spring 2006 70
I Leads V???What the **(&@ does that mean??
I
V
Current reaches it’s maximum at an earlier time than the voltage!
1
2
I = C VP sin (t +/2)
Phase=
-(/2)
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Induction - Spring 2006 71
Capacitor Example
E
~
CA 100 nF capacitor isconnected to an AC supply of peak voltage 170V and frequency 60 Hz.
What is the peak current?What is the phase of the current?
MX
f
C 65.2C
1
1077.3C
rad/sec 77.360227
Also, the current leads the voltage by 90o (phase difference).
I=V/XC
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Induction - Spring 2006 72
Again this looks like IP=VP/R for aresistor (except for the phase change).
So we call XL = L the Inductive Reactance
Inductors in AC Circuits
LV = VP sin (t)Loop law: V +VL= 0 where VL = -L dI/dtHence: dI/dt = (VP/L) sin(t).Integrate: I = - (VP / L cos (t)
or I = [VP /(L)] sin (t - /2)
~
Here the current lags the voltage by 90o.
V
t
I
V and I “out of phase” by 90º. I lags V by 90º.
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Induction - Spring 2006 73
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Induction - Spring 2006 74
Phasor Diagrams
Vp
Ipt
Resistor
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.
The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.
Phasor diagrams are useful in solving complex AC circuits.The “y component” is the actual voltage or current.
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.
The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.
Phasor diagrams are useful in solving complex AC circuits.The “y component” is the actual voltage or current.
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Induction - Spring 2006 75
Phasor Diagrams
Vp
Ipt
Vp
Ip
t
Resistor Capacitor
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.Phasor diagrams are useful in solving complex AC circuits.The “y component” is the actual voltage or current.
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.Phasor diagrams are useful in solving complex AC circuits.The “y component” is the actual voltage or current.
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Induction - Spring 2006 76
Phasor Diagrams
Vp
Ipt
Vp
IpVp Ip
Resistor Capacitor Inductor
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.Phasor diagrams are useful in solving complex AC circuits.The “y component” is the actual voltage or current.
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.Phasor diagrams are useful in solving complex AC circuits.The “y component” is the actual voltage or current.
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Induction - Spring 2006 77
Steady State Solution for AC Current (2)
• Expand sin & cos expressions
• Collect sindt & cosdt terms separately
• These equations can be solved for Im and (next slide)
1/ cos sin 0
1/ sin cos
d d
m d d m m
L C R
I L C I R
sin sin cos cos sin
cos cos cos sin sin
d d d
d d d
t t t
t t t
High school trig!
cosdt terms
sindt terms
cos sin cos sinmm d d m d d m d
d
II L I R t t t
C
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Induction - Spring 2006 78
Steady State Solution for AC Current (2)
• Expand sin & cos expressions
• Collect sindt & cosdt terms separately
• These equations can be solved for Im and (next slide)
1/ cos sin 0
1/ sin cos
d d
m d d m m
L C R
I L C I R
sin sin cos cos sin
cos cos cos sin sin
d d d
d d d
t t t
t t t
High school trig!
cosdt terms
sindt terms
cos sin cos sinmm d d m d d m d
d
II L I R t t t
C
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Induction - Spring 2006 79
• Solve for and Im in terms of
• R, XL, XC and Z have dimensions of resistance
• Let’s try to understand this solution using “phasors”
Steady State Solution for AC Current (3)
1/tan d d L CL C X X
R R
m
mIZ
22L CZ R X X
L dX L
1/C dX CInductive “reactance”
Capacitive “reactance”
Total “impedance”
1/ cos sin 0
1/ sin cos
d d
m d d m m
L C R
I L C I R
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Induction - Spring 2006 80
REMEMBER Phasor Diagrams?
Vp
Ipt
Vp
Ip
t
Vp Ip
t
Resistor Capacitor Inductor
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.Phasor diagrams are useful in solving complex AC circuits.
A phasor is an arrow whose length represents the amplitude ofan AC voltage or current.The phasor rotates counterclockwise about the origin with the angular frequency of the AC quantity.Phasor diagrams are useful in solving complex AC circuits.
![Page 81: Induction - Spring 20061 Time Varying Circuits April 10, 2006.](https://reader036.fdocuments.us/reader036/viewer/2022062304/56649e9d5503460f94b9d742/html5/thumbnails/81.jpg)
Induction - Spring 2006 81
Reactance - Phasor Diagrams
Vp
Ipt
Vp
Ip
t
Vp Ip
t
Resistor Capacitor Inductor
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Induction - Spring 2006 82
“Impedance” of an AC Circuit
R
L
C~
The impedance, Z, of a circuit relates peakcurrent to peak voltage:
IV
Zpp (Units: OHMS)
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Induction - Spring 2006 83
“Impedance” of an AC Circuit
R
L
C~
The impedance, Z, of a circuit relates peakcurrent to peak voltage:
IV
Zpp (Units: OHMS)
(This is the AC equivalent of Ohm’s law.)
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Induction - Spring 2006 84
Impedance of an RLC Circuit
R
L
C~E
As in DC circuits, we can use the loop method:
E - VR - VC - VL = 0 I is same through all components.
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Induction - Spring 2006 85
Impedance of an RLC Circuit
R
L
C~E
As in DC circuits, we can use the loop method:
E - VR - VC - VL = 0 I is same through all components.
BUT: Voltages have different PHASES
they add as PHASORS.
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Induction - Spring 2006 86
Phasors for a Series RLC Circuit
Ip
VRp
(VCp- VLp)
VP
VCp
VLp
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Induction - Spring 2006 87
Phasors for a Series RLC Circuit
By Pythagoras’ theorem:
(VP )2 = [ (VRp )2 + (VCp - VLp)2 ]
Ip
VRp
(VCp- VLp)
VP
VCp
VLp
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Induction - Spring 2006 88
Phasors for a Series RLC Circuit
By Pythagoras’ theorem:
(VP )2 = [ (VRp )2 + (VCp - VLp)2 ]
= Ip2 R2 + (Ip XC - Ip XL)
2
Ip
VRp
(VCp- VLp)
VP
VCp
VLp
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Induction - Spring 2006 89
Impedance of an RLC Circuit
Solve for the current:
Ip Vp
R2 (Xc XL )2
Vp
Z
R
L
C~
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Induction - Spring 2006 90
Impedance of an RLC Circuit
Solve for the current:
Impedance:
Ip Vp
R2 (Xc XL )2
Vp
Z
Z R2 1
C L
2
R
L
C~
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Induction - Spring 2006 91
The circuit hits resonance when 1/C-L=0: r=1/When this happens the capacitor and inductor cancel each otherand the circuit behaves purely resistively: IP=VP/R.
Impedance of an RLC Circuit
Ip Vp
Z
Z R2 1
C L
2
The current’s magnitude depends onthe driving frequency. When Z is aminimum, the current is a maximum.This happens at a resonance frequency:
LC
The current dies awayat both low and highfrequencies.
IP
01 0
21 0
31 0
41 0
5
R = 1 0 0
R = 1 0
r
L=1mHC=10F
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Induction - Spring 2006 92
Phase in an RLC CircuitIp
VRp
(VCp- VLp)
VP
VCp
VLp
We can also find the phase:
tan = (VCp - VLp)/ VRp
or; tan = (XC-XL)/R.
or tan = (1/C - L) / R
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Induction - Spring 2006 93
Phase in an RLC Circuit
At resonance the phase goes to zero (when the circuit becomespurely resistive, the current and voltage are in phase).
IpVRp
(VCp- VLp)
VP
VCp
VLp
We can also find the phase:
tan = (VCp - VLp)/ VRp
or; tan = (XC-XL)/R.
or tan = (1/C - L) / R
More generally, in terms of impedance:
cos R/Z
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Induction - Spring 2006 94
Power in an AC Circuit
V(t) = VP sin (t)
I(t) = IP sin (t)
P(t) = IV = IP VP sin 2(t) Note this oscillates
twice as fast.
V
t
I
t
P
= 0
(This is for a purely resistive circuit.)
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Induction - Spring 2006 95
The power is P=IV. Since both I and V vary in time, sodoes the power: P is a function of time.
Power in an AC Circuit
Use, V = VP sin (t) and I = IP sin (t+) :
P(t) = IpVpsin(t) sin (t+)
This wiggles in time, usually very fast. What we usually care about is the time average of this:
PT
P t dtT
10
( ) (T=1/f )
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Induction - Spring 2006 96
Power in an AC Circuit
Now: sin( ) sin( )cos cos( )sin t t t
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Induction - Spring 2006 97
Power in an AC Circuit
P t I V t tI V t t t
P P
P P
( ) sin( )sin( )sin ( )cos sin( )cos( )sin
2
Now: sin( ) sin( )cos cos( )sin t t t
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Induction - Spring 2006 98
Power in an AC Circuit
P t I V t tI V t t t
P P
P P
( ) sin( )sin( )sin ( )cos sin( )cos( )sin
2
sin ( )
sin( ) cos( )
2 1
2
0
t
t t
Use:
and:
So P I VP P1
2cos
Now: sin( ) sin( )cos cos( )sin t t t
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Induction - Spring 2006 99
Power in an AC Circuit
P t I V t tI V t t t
P P
P P
( ) sin( )sin( )sin ( )cos sin( )cos( )sin
2
sin ( )
sin( ) cos( )
2 1
2
0
t
t t
Use:
and:
So P I VP P1
2cos
Now:
which we usually write as P I Vrms rms cos
sin( ) sin( )cos cos( )sin t t t
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Induction - Spring 2006 100
Power in an AC Circuit
P I Vrms rms cos goes from -900 to 900, so the average power is positive)
cos( is called the power factor.
For a purely resistive circuit the power factor is 1.When R=0, cos()=0 (energy is traded but not dissipated).Usually the power factor depends on frequency.