Node Analysis, With and Without Voltage Sources - Lecture Slides | ECE 2040, Study notes of Electrical Circuit Analysis

Material Type: Notes; Class: Circuit Analysis; Subject: Electrical & Computer Engr; University: Georgia Institute of Technology-Main Campus; Term: Unknown 1989;

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Pre 2010

Uploaded on 08/04/2009

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Circuit Analysis Lecture #5
Outline:
โ€ขNode analysis
โ€ขWithout voltage sources
โ€ขWith voltage sources
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Download Node Analysis, With and Without Voltage Sources - Lecture Slides | ECE 2040 and more Study notes Electrical Circuit Analysis in PDF only on Docsity!

Circuit Analysis Lecture

Outline:

  • Node analysis
  • Without voltage sources
  • With voltage sources

Circuit Equations

  • Method #1:
  • Apply KVL & KCL as needed
  • Result: Set of simultaneous equations

Ax = b where A is a matrix, b is a column vector, and x is a column vector of unknown volt- ages/currents.

  • Pros: Straightforward & guaranteed
  • Cons: Cumbersome (on paper) & results in additional variables & equations
  • Alternatives:
    • Node analysis
    • Mesh analysis
  • Can view these as โ€œguidedโ€ KVL & KCL

Illustration

  • From previous figure...two nodes plus reference
  • What is voltage across resistor R 1?
    • Let vab denote differential with a positive and b negative va โˆ’ vab โˆ’ vb = 0 โ‡’ va โˆ’ vb = vab
    • Let vba denote differential with a negative and b positive va + vba โˆ’ vb = 0 โ‡’ vba = vb โˆ’ va
  • What is current through resistor R 1?
    • From a to b: vab/R 1
    • From b to a: vba/R 2
  • To determine va & vb:
    • KCL at a: is = va/R 2 + (va โˆ’ vb)/R 1
    • KCL at b: (va โˆ’ vb)/R 1 = vb/R 3
  • 2 equations for 2 unknowns...

Node Voltage Relationships

  • KVL: v 12 = v 1 โˆ’ v 2
  • In case of voltage source between nodes: v 12 = Vs (subject to consistent signs)
  • In case of resistor between nodes: i = (v 1 โˆ’ v 2 )/R (from 1 to 2 )

Example with Voltage Source

  • Node a: 3 branches va/R 1 + (va โˆ’ vb)/R 2 +? = 0
  • On one hand: Cannot immediately compute current through vs
  • On other hand: Know va = vs, so only unknown node voltage is vb
  • Node b: 3 branches (vb โˆ’ va)/R 2 + vb/R 3 = is
  • Substitute va = vs and solve for vb
  • KCL at node a provides current through voltage source

Example with Voltage Source, cont

  • Node a: va/R 1 +? = 0
  • Node b: vb/R 2 +? = is
  • Unlike previous example, we only know relative voltage

va โˆ’ vb = vs but not absolute value of va or vb

  • Solution: Apply KCL to union of nodes, i.e., โ€œsupernodeโ€

va/R 1 + vb/R 2 = is

  • This is shortcut to labeling & eliminating current through voltage source

More Examples

  • ab : 1.5 = va/6 + 3.5 + vb/ 3
  • ab : vb โˆ’ va = 12
  • a : va = 8
  • b : (vb โˆ’^ va)/6 + (vb โˆ’^ vc)/3 = 2
  • c : vc = 3ix
  • ix = (va โˆ’ vb)/ 6

More Examples, cont

  • ab : 3 = va/4 + vb/ 10
  • va โˆ’ vb = 4vx
  • vx = โˆ’va
  • a : (va โˆ’ 6)/10 + ia + (va โˆ’ vb)/20 = 0
  • b : (vb โˆ’ va)/20 + 5ia = 0
  • ia = (6 โˆ’ va)/10 + (vb โˆ’ va)/ 20