AC#Circuits - SFU.ca Lecture 20 - AC... · 2013-06-28 · Other#videos:...
Transcript of AC#Circuits - SFU.ca Lecture 20 - AC... · 2013-06-28 · Other#videos:...
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AC CircuitsMaximum currents & voltages
Phasors: A Simple Tool
Electricity & MagnetismLecture 20
Today’s Concept:
Electricity & Magne?sm Lecture 20, Slide 1
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Other videos:
Prof. W. Lewin, MIT Open Courseware
Mechanical Universe, Driven LRC circuits
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Resistors
R I = VR/R = Vmax/R sin(ωt)
Amplitude = Vmax/R
ε = Vmaxsin(ωt)
Electricity & Magne?sm Lecture 20, Slide 3
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Capacitors
C I = VmaxωC cos(ωt)
where XC = 1/ωCis like the “resistance”of the capacitor XC depends on ω
Amplitude = Vmax/XC
I = dQ/dt
Q = CV = CVmaxsin(ωt)
90o
ε = Vmaxsin(ωt)
Electricity & Magne?sm Lecture 20, Slide 4
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Inductors
L I = − (Vmax/ωL) cos(ωt)
Amplitude = Vmax/XL
where XL = ωLis like the “resistance”of the inductor XL depends on ω
dI/dt = VL = Vmaxsin(ωt)
90o
ε = Vmaxsin(ωt)
Electricity & Magne?sm Lecture 20, Slide 5
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RL Clicker Question
An RL circuit is driven by an AC generator as shown in the figure.
For what driving frequency ω of the generator will the current through the resistor be largest A) ω largeB) Current through R doesn’t depend on ω C) ω small
L
R
XL = ωL
As ω → 0, so does XL
As ω → 0, resistance of circuit → Rcurrent gets bigger
Electricity & Magne?sm Lecture 20, Slide 6
impedance
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R Imax = Vmax/R VR in phase with I
L Imax = Vmax/XL VL 90o ahead of IXL = ωL
C Imax = Vmax/XC VC 90o behind IXC = 1/ωC Current comes first since it
charges capacitor
Because resistors are simple
Opposite of capacitor
Like a wire at high ω
Like a wire at low ω
Summary
Electricity & Magne?sm Lecture 20, Slide 7
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Vmax = Imax XL
Vmax = Imax XC
Vmax = Imax RV in phase with I
V 90o behind I
V 90o ahead of I
Makes sense to write everything in terms of I since this is the same everywhere in a one-‐loop circuit: Imax XL
Imax XC
Imax R
Phasors make this simple to see
Always looks the same. Only the lengths will change
εmax
“Do you have any fancy-‐schmancy simula?ons for to show me?”
Electricity & Magne?sm Lecture 20, Slide 8
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Imax XL
Imax XC
Imax R Imax XL
Imax R
Imax XC
εmax
But now we are adding vectors:
Imax XL
Imax XC
Imax R
εmax
The Voltages still Add Up
Electricity & Magne?sm Lecture 20, Slide 9
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Imax XL
Imax XC
Imax R
εmax
Make this Simpler
Imax XL
Imax XC
Imax R
Electricity & Magne?sm Lecture 20, Slide 10
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Imax R
εmax = Imax ZImax(XL − XC)
Make this Simpler
Imax XL
Imax XC
Imax R
Electricity & Magne?sm Lecture 20, Slide 11
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Imax R
εmax = Imax Z
Imax(XL − XC)
Make this Simpler
Electricity & Magne?sm Lecture 20, Slide 12
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Imax R
εmax = Imax Z
Imax(XL − XC)
R(X
L − XC )
φ
φ
Impedance Triangle
Make this Simpler
Electricity & Magne?sm Lecture 20, Slide 13
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φ
R (XL − X
C )
VCmax = Imax XC
VLmax = Imax XL
VRmax = Imax R
Summary
Imax = εmax / Z
εmax = Imax Z
Electricity & Magne?sm Lecture 20, Slide 14
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Imax XL
Imax R
εmax
Example: RL Circuit Xc = 0
Electricity & Magne?sm Lecture 20, Slide 15
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0
15
30
45
60
1
ABC
Draw Voltage Phasors
CheckPoint 2
Imax XL
Imax R
εmax
Electricity & Magne?sm Lecture 20, Slide 16
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0
15
30
45
60
1
ABC
CheckPoint 4
Draw Voltage PhasorsImax XL
Imax R
εmax
Electricity & Magne?sm Lecture 20, Slide 17
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0
13
25
38
50
1
The CURRENT is THE CURRENT
ABCD
φ is the phase between generator and current
φ
CheckPoint 6
Imax XL
Imax R
εmax
Electricity & Magne?sm Lecture 20, Slide 18
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CheckPoint 8
0
13
25
38
50
1
ABC
What does the voltage phasor diagram look like when the current is a maximum?
IXc
IRε
IXL
IXc
IR
εIXL
Electricity & Magne?sm Lecture 20, Slide 19
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0
13
25
38
50
1
What does the voltage phasor diagram look like when the capacitor is fully charged?
ABC
IXc
IRε
IXL
IXc
IR
εIXL
CheckPoint 10
Electricity & Magne?sm Lecture 20, Slide 20
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CheckPoint 12
0
13
25
38
50
1
What does the voltage phasor diagram look like when the voltage across capacitor is at its posi?ve maximum?
ABC
IXc
IRε
IXL
IXc
IR
εIXL
Electricity & Magne?sm Lecture 20, Slide 21
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Conceptual AnalysisThe maximum voltage for each component is related to its reactance and to the
maximum current.The impedance triangle determines the rela?onship between the maximum
voltages for the components Strategic Analysis
Use Vmax and Imax to determine ZUse impedance triangle to determine R Use VCmax and impedance triangle to determine XL
~
C
RLV
Calculation
Electricity & Magne?sm Lecture 20, Slide 22
Consider the harmonically driven series LCR circuit shown. Vmax = 100 VImax = 2 mAVCmax = 113 VThe current leads generator voltage by 45o
L and R are unknown.
What is XL, the reactance of the inductor, at this frequency?
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Compare XL and XC at this frequency:
A) XL < XC B) XL = XC C) XL > XC D) Not enough informa?on
This informa?on is determined from the phaseCurrent leads voltage
VL = ImaxXLVC = ImaxXC
VR (phase of current)
VL
VC V leads
IR
V
45ο
Calculation
~
C
RLV
Electricity & Magne?sm Lecture 20, Slide 23
Consider the harmonically driven series LCR circuit shown. Vmax = 100 VImax = 2 mAVCmax = 113 VThe current leads generator voltage by 45o
L and R are unknown.
What is XL, the reactance of the inductor, at this frequency?
![Page 24: AC#Circuits - SFU.ca Lecture 20 - AC... · 2013-06-28 · Other#videos: Prof.#W.#Lewin,#MIT#Open#Courseware Mechanical#Universe,#Driven#LRC#circuits](https://reader033.fdocuments.in/reader033/viewer/2022041815/5e5a1d8e2a14a32868253a38/html5/thumbnails/24.jpg)
What is Z, the total impedance of the circuit?
A) B) C) D)35.4 kΩ50 kΩ 21.1 kΩ70.7 kΩ
Calculation
~
C
RLV
Electricity & Magne?sm Lecture 20, Slide 24
Consider the harmonically driven series LCR circuit shown. Vmax = 100 VImax = 2 mAVCmax = 113 VThe current leads generator voltage by 45o
L and R are unknown.
What is XL, the reactance of the inductor, at this frequency?
![Page 25: AC#Circuits - SFU.ca Lecture 20 - AC... · 2013-06-28 · Other#videos: Prof.#W.#Lewin,#MIT#Open#Courseware Mechanical#Universe,#Driven#LRC#circuits](https://reader033.fdocuments.in/reader033/viewer/2022041815/5e5a1d8e2a14a32868253a38/html5/thumbnails/25.jpg)
What is R?A) B) C) D)
Z = 50 kΩ
sin(45°) =0.707
cos(45°) =0.70735.4 kΩ50 kΩ 21.1 kΩ70.7 kΩ
= 50 kΩ × 0.707
= 35.4 kΩ
Calculation
~
C
RLV
Determined from impedance triangleR
Z = 50kΩ
(XC − XL)45ο R = Z cos(45o)
Electricity & Magne?sm Lecture 20, Slide 25
Consider the harmonically driven series LCR circuit shown. Vmax = 100 VImax = 2 mAVCmax = 113 VThe current leads generator voltage by 45o
L and R are unknown.
What is XL, the reactance of the inductor, at this frequency?
![Page 26: AC#Circuits - SFU.ca Lecture 20 - AC... · 2013-06-28 · Other#videos: Prof.#W.#Lewin,#MIT#Open#Courseware Mechanical#Universe,#Driven#LRC#circuits](https://reader033.fdocuments.in/reader033/viewer/2022041815/5e5a1d8e2a14a32868253a38/html5/thumbnails/26.jpg)
A) B) C) D)
Z = 50 kΩ
R = 35.4kΩ
What is XC?
35.4 kΩ50 kΩ 21.1 kΩ70.7 kΩ
VCmax = ImaxXC
Calculation
Consider the harmonically driven series LCR circuit shown. Vmax = 100 VImax = 2 mAVCmax = 113 VThe current leads generator voltage by 45o
L and R are unknown.
What is XL, the reactance of the inductor, at this frequency?
~
C
RLV
XL = XC − R
XL = 56.5 kΩ − 35.4 kΩ
R
Z(XC − XL)
45ο
We start with the impedance triangle:
Electricity & Magne?sm Lecture 20, Slide 26
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Practical Test Hints
You will have 4 banana plug wires, ~4 alligator clips 1 Scope Probe (x1/x10) 1 BNC wire adaptors: Tee, BNC-‐Male Banana, BNC-‐Female Banana proto-‐board (Use it!) scope, func?on generator, DMM
We will have two 60 min sessions: 12:30 — 13:30 13:40 — 14:30