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ELECTRIC CIRCUITS ECSE2010 Spring 2003 Class 5

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Used to Model Electronic Devices. Make Circuits Interesting (and Harder) Equivalent Resistance: ... KCL and KVL. Simplify Circuits using Series/Parallel R's ... – PowerPoint PPT presentation

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Title: ELECTRIC CIRCUITS ECSE2010 Spring 2003 Class 5


1
ELECTRIC CIRCUITSECSE-2010Spring 2003 Class 5

2
ASSIGNMENTS DUE
  • Today (Thursday)
  • Activities 5-1, 5-2, 5-3 (In Class)
  • Next Monday
  • HW 2 Due
  • Experiment 1 Report Due
  • Activities 6-1, 6-2, 6-3, 6-4 (In Class)
  • Next Tuesday/Wednesday
  • Will do Experiment 2 In Class (EP-2)
  • Activities 7-1, 7-2, (In Class)

3
REVIEW
  • Controlled/Dependent Sources
  • VCVS, VCCS, CCVS, CCCS
  • Used to Model Electronic Devices
  • Make Circuits Interesting (and Harder)
  • Equivalent Resistance
  • Replace any Load Network with Req
  • Load Network Rs, Controlled Sources, No
    Independent Sources

4
CONTROLLED SOURCES
5
CONTROLLED SOURCES
6
CONTROLLED SOURCES
7
CONTROLLED SOURCES
8
EQUIVALENT RESISTANCE
9
Req with Controlled Sources
10
REVIEW
  • Req with Controlled Sources
  • Connect Test Voltage vt
  • Define it Using Active Convention
  • Find it in terms of vt (Use KCL, KVL, Ohms Law,
    etc.)
  • Req vt / it

11
WHERE ARE WE?
  • Circuit Elements
  • Ideal, Independent i and v sources
  • Ideal, Controlled i and v sources
  • Resistors
  • Potentiometers
  • Have Learned How to Define all is and vs using
    Active/Passive Convention
  • Have Begun to do Circuit Analysis Solving for
    all is and vs

12
WHERE ARE WE?
  • Circuit Analysis Techniques
  • Ohms Law for Rs
  • KCL and KVL
  • Simplify Circuits using Series/Parallel Rs
  • Replace Load Network with Req
  • Sometimes Hard to Know Where to Start
  • Will Now Develop Systematic Techniques that will
    Always Work
  • Node Equations Today
  • Mesh Equations on Monday

13
NODE EQUATIONS
  • Systematic Technique for Solving ANY Linear
    Circuit
  • Will Always Work!
  • Not Always the Easiest Technique
  • Will Also Learn About Mesh Equations
  • Can Use Either Technique But Cannot Mix
  • Very Powerful Techniques!!
  • Will Use For Rest of Course

14
EXAMPLE
15
NODE EQUATIONS
  • See Example Ckt
  • Node Equation Procedure
  • Label Unknown Node Voltages (v1, v2, )

16
EXAMPLE
17
NODE EQUATIONS
  • Node Equation Procedure
  • Label Unknown Node Voltages (v1, v2, )
  • of Unknown Node Voltages of Nodes - of
    Voltage Sources - 1 (Reference)
  • Example 4 Nodes - 1 Voltage Source - 1 2
    Unknown Node Voltages v1, v2
  • Write a KCL at Each Unknown Node Voltage
  • Sum of Currents Out 0
  • Express is in terms of Node Voltages

18
EXAMPLE
19
NODE EQUATIONS
  • Example

20
NODE EQUATIONS
  • Example

21
NODE EQUATIONS
  • Writing a KCL at Each Unknown Node Voltage will
    Always Provide of Linear Equations
    Unknowns
  • Can Always Solve for v1, v2, .
  • Node Equations will ALWAYS work
  • Can take it to the bank

22
ACTIVITY 5-1

23
ACTIVITY 5-1
  • 6 Nodes - 2 Voltage Sources - 1 (Ref)
  • gt 3 Unknown Node Voltages
  • v1, v2, v3

24
ACTIVITY 5-1

25
ACTIVITY 5-1
  • 6 Nodes - 2 Voltage Sources - 1 (Ref)
  • gt 3 Unknown Node Voltages
  • v1, v2, v3
  • Write a KCL at each Unknown Node Voltage,
    relating Currents to the Node Voltages using
    Ohms Law
  • Usually best to sum Currents OUT of the Node

26
ACTIVITY 5-1

27
ACTIVITY 5-1
28
ACTIVITY 5-1
29
ACTIVITY 5-1
30
ACTIVITY 5-1
31
ACTIVITY 5-2
  • For Large Matrices, Use MAPLE
  • Usually for n gt 2
  • Must Include with (linalg)
  • Two Ways to Solve using MAPLE
  • See MAPLE Scripts
  • Must Be Careful with Syntax

32
ACTIVITY 5-2
  • MAPLE SCRIPT Classic Method
  • gtwith (linalg)
  • gtGR-gtmatrix(3,3,1/51/101/R,
    -1/R,-1/10,-1/R,1/201/41/R,0,
    -1/10,0,1/10)
  • gtG(R)
  • gtIsmatrix(3,1,14,-10,-2)

33
ACTIVITY 5-2
  • gtvR-gtevalm(inverse(G(R))Is)
  • means matrix multiplication
  • gtv(R)
  • gtv(1)
  • gtiaR-gt(v(R)2,1-2)
  • gtia(R)
  • gtia(1)

34
ACTIVITY 5-2
  • MAPLE SCRIPT Gaussjord Method
  • gtwith (linalg)
  • gtGR-gtmatrix(3,4,1/51/101/R,
    -1/R,-1/10,14,-1/R,1/201/41/R,0,
    -10,-1/10,0,1/10,-2)
  • gtG(R)
  • gtBR-gtguassjord(G(R))
  • gtB(R)
  • leads to same result

35
ACTIVITY 5-3a
36
ACTIVITY 5-3a
  • KCL at Node v
  • Sum of Currents Out of Node 0
  • (v-30)/6 (v8)/2 (v8-30)/10 - 5 0
  • v (1/6 1/2 1/10) 30/6 8/2 22/10 5
  • gt (23/30) v 8.2 gt v 10.7 V
  • Writing a KCL at each Unknown Node always works!

37
ACTIVITY 5-3b
38
ACTIVITY 5-3b
  • 5 Nodes - 2 Voltage Sources - 1 (Ref)
  • 2 Unknown Node Voltages, v1, v2
  • Write a KCL at each Unknown Node
  • Sum of Currents Out 0

39
ACTIVITY 5-3b
40
ACTIVITY 5-3b
41
ACTIVITY 5-3b
42
ACTIVITY 5-3b
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