review of lectures 05-08review of lectures 05-08 07/23/2013 ece225 circuit analysis. contents of...
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CIRCUITS by Ulaby & MaharbizAll rights reserved. Do not reproduce or distribute.
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REVIEW OF LECTURES 05-08REVIEW OF LECTURES 05 08
07/23/2013 ECE225 CIRCUIT ANALYSIS
Contents of Midterm #2Midterm #2 Schecule: 10:45~13:15 July 25 Thursday
L t 05 08
Midterm #2 Schecule: 10:45 13:15, July 25, Thursday
Sections 3.5-3.6; 4.3-4.7; 5.2-5.3. Lectures 05-08 Sections 3.5 3.6; 4.3 4.7; 5.2 5.3.
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Summary of Chapter 3 (part 3)y p (p )
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Thévenin’s Theorem
Linear two-terminal circuit can be replaced by an
equivalent circuit composed of a voltage
source and a series resistor
voltage across output with no load (open circuit)
inTh RR
Resistance at terminals with all Resistance at terminals with all independent circuit sources set to zero
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Norton’s TheoremAll rights reserved. Do not reproduce or distribute. © 2013 National Technology and Science Press
Linear two-terminal circuit can be replaced by an equivalent be replaced by an equivalent circuit composed of a current source and parallel resistor
Current through output with short circuit
Resistance at terminals with all circuit sources set to zero
How Do We Find Thévenin/Norton E i l t Ci it ?Equivalent Circuits ? Method 1: Open circuit/Short circuit Method 1: Open circuit/Short circuit
1. Analyze circuit to find
2. Analyze circuit to find
Note: This method is applicable to Note: This method is applicable to any circuit, whether or not it contains dependent sources.
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Example 3-10: Thévenin Equivalent All rights reserved. Do not reproduce or distribute. © 2013 National Technology and Science Press
p q
How Do We Find Thévenin/Norton E i l t Ci it ?Equivalent Circuits?Method 2: Equivalent ResistanceMethod 2: Equivalent Resistance
1. Analyze circuit to find either
or 2 ll d d b2. Deactivate all independent sources by replacing voltage sources with short circuits and current sources with open circuits.3. Simplify circuit to find equivalent resistance
Note: This method does not apply to circuits that contain dependent sources.p
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Example 3-11: RTh
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p Th
(Ci i h d d )Replace with SC (Circuit has no dependent sources)
Replace with OC
How Do We Find Thévenin/Norton E i l t Ci it ?Equivalent Circuits?
Method 3:
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ExampleExample All rights reserved. Do not
reproduce or distribute. © 2013 National Technology
and Science Press p
E l ( t )
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To find
Example (cont.)
Power TransferAll rights reserved. Do not reproduce or distribute. © 2013 National Technology and Science Press
In many situations, we want to y ,maximize power transfer to the load
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and Science Press
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Summary of Chapter 4y p
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Circuit Analysis With Ideal Op AmpsAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
y p p
Use nodal analysis as before, but with “golden rules”
N No current into op amp
No voltage drop across op amp input
Do not apply KCL at op amp output
Noninverting Amplifierg p
At node
021
Rv
Rvv non
spn vvv
so vR
RRv2
21
(max) = Vcc
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Inverting Amplifierg p
0 pn vv
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Example 4-2: Input Current SourceAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
p pRelate output voltage to input current sourcep
Summing Amplifierg p
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Example 4-3: p
Solution:
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Difference AmplifierAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
p
Note negative gain of channel 1
Voltage FollowerAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
g
“Buffers” Sections of CircuitBuffers Sections of Circuit
depends on both input and load iresistors
is immune to input and load resistors
What is the op amp doing?
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Summary of Chapter 5 (Parts 1)All rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
y p ( )
CapacitorsAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
p
Passive element that stores energy in electric fieldPassive element that stores energy in electric field
Parallel plate capacitor
AdAC
0 1 tdtit
0oC t
For DC, capacitor looks like open circuitlike open circuit
Voltage on capacitor must be continuous (no abrupt change)abrupt change)
Energy Stored in Capacitorgy p
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Capacitor Response: Given v(t), determine i(t), p(t), and w(t)
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C = C =
RC Circuits at dcAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
At dc no currents flow through capacitors: open circuits At dc no currents flow through capacitors: open circuits
Capacitors in Seriesp
Use KVL, current same ,through each capacitor
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Capacitors in Parallelp
Use KCL, voltage same , gacross each capacitor
NCCCCC 321eq
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Voltage Divisiong
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InductorsAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
Passive element that stores energy in magnetic fieldgy g
Solenoid Wound Inductor
0o
1 tidttvL
it
t
At dc, inductor looks like a short circuit
Current through inductor Current through inductor must be continuous (no abrupt change)
AN 2
lANL 2
Inductor Response to p
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Inductors in Series
Use KVL, current is same ,through all inductors
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Inductors in Parallel
V lt i ll Voltage is same across all inductors
Inductors add together in the same way resistors do
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RL Circuits at dcAll rights reserved. Do not copy or distribute. © 2013 National Technology and Science Press
At dc no voltage across inductors: short circuit At dc no voltage across inductors: short circuit
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