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LN3 Geng2340

This document provides an overview of nodal analysis and mesh analysis techniques for circuit analysis. It discusses: 1) The steps of nodal analysis including selecting a reference node, applying Kirchhoff's Current Law to write nodal equations, and solving the equations to find node voltages. 2) How to handle circuits with voltage sources by setting node voltages equal to source voltages or applying KCL and KVL to supernodes. 3) Mesh analysis involves assigning mesh currents, applying Kirchhoff's Voltage Law to write mesh equations, and solving for unknown mesh currents. It is only applicable to planar circuits that can be redrawn without crossing branches.

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0% found this document useful (0 votes)
161 views61 pages

LN3 Geng2340

This document provides an overview of nodal analysis and mesh analysis techniques for circuit analysis. It discusses: 1) The steps of nodal analysis including selecting a reference node, applying Kirchhoff's Current Law to write nodal equations, and solving the equations to find node voltages. 2) How to handle circuits with voltage sources by setting node voltages equal to source voltages or applying KCL and KVL to supernodes. 3) Mesh analysis involves assigning mesh currents, applying Kirchhoff's Voltage Law to write mesh equations, and solving for unknown mesh currents. It is only applicable to planar circuits that can be redrawn without crossing branches.

Uploaded by

Seth Vineet
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
You are on page 1/ 61

Electrical and Computing Fundamentals

GENG 2340

Dr. A. Emadi
Department of Electrical and Computer Engineering

1
Methods of Analysis
• Nodal Analysis
• Nodal Analysis with Voltage Sources
• Mesh Analysis
• Mesh Analysis with Current Sources
• Nodal Versus Mesh Analysis

Chapter #3
Images and Texts are from the course textbook @ McGraw-Hill and Wiley, Refer to Syllabus
Fundamentals of Electric Circuits by C. Alexander and M. Sadiku, 7th Edition
Fundamentals of Electric Circuit Analysis by C. R. Paul
2
Introduction
Use three laws (Ohm’s, KCL, KVL) to develop two analysis
techniques:
1) Nodal analysis
• Systematic application of KCL
• Write nodal equations
• Solve for unknown node voltages
2) Mesh analysis
• Systematic application of KVL
• Write mesh equations
• Solve for unknown mesh/loop currents
Obtain a set of simultaneous equations that can be solved to
obtain the values of current or voltage. 3
Nodal Analysis
• Node – Voltage method
• General procedure for analyzing circuits using node voltages:
• Use node voltages (referenced to ground or another node) instead of
element voltages as it is convenient and reduces the number of
simultaneous equations
• Interested in finding the node voltages

4
Nodal Analysis – Steps
1) Setup Circuit
• Select a node as the reference node
• Assign voltages v1,v2,…,vn-1 to the remaining n-1 nodes
• Voltages are referenced with respect to the reference node
2) Setup Equations
• Apply KCL to each of the non-reference nodes
• Use Ohm’s law to express the branch currents in terms of node
voltages
3) Solve the resulting simultaneous equations
• Solve to obtain the unknown node voltages

5
Nodal Analysis – Step 1
• Select a reference node (e.g. the
ground, zero potential, node 0).

• All voltages will be referenced from


this node.

• Few symbols:
• a – common ground
• b – ground
• c – chassis ground

6
Nodal Analysis – Step 2
• Nodes 1 and 2 are assigned voltages v1 and
v2 respectively.
• Redraw circuit to include only node voltages
and currents at these nodes
• Apply KCL to each non-reference node.
• Add currents through resistors.

I1 = I 2 + i1 + i2 at 1
I 2 + i2 = i3 at 2
7
Nodal Analysis – Step 2
• Apply Ohm’s Law to unknown currents: i1, i2 and i3
• Current flows from a higher potential to a lower
potential
• Choose a direction for current
• Label the current
• Voltage at the beginning of arrow minus voltage at the
end of the arrow divided by R

8
Nodal Analysis – Step 2
• Substituting back to the original nodal
equations:
v1 v1 - v2
I1 = I 2 + +
R1 R2
v1 - v2 v2
I2 + =
R2 R3
or
I1 = I 2 + v1G1 + (v1 - v2 )G2
I 2 + (v1 - v2 )G2 = v2G3
9
Nodal Analysis – Step 2
• Place equations in matrix form:

éG1 + G2 -G2 ù é v1 ù é I1 - I 2 ù
ê -G ú ê ú =ê ú
ë 2 G2 + G3 û ëv2 û ë I 2 û
from
I1 = I 2 + v1G1 + (v1 - v2 )G2
I 2 + (v1 - v2 )G2 = v2G3

10
Nodal Analysis – Step 3
• Use Cramer’s Rule

éa b ù é e ù é g ù
êc d ú ê f ú = ê h ú
ë ûë û ë û
D = ad - cb
D1 = gd - hb D 2 = ah - cg
D1 D2
e= f =
D D
• For 2x2 only!
11
Nodal Analysis
(a) a general circuit
(b) definition of the node voltages
(c) labeling of the original circuit with the node voltages.

12
Example #1 – Nodal Analysis
Find V2:

13
Example #2 – Nodal Analysis
Applying KCL at node 1 gives:

14
Example #2 Cont. – Nodal Analysis
Applying KCL at node 2 gives:

15
Example #2 Cont. – Nodal Analysis
Calculate v1 and v2.

16
Example #3 – Nodal Analysis
Calculate I.
Solution: assume d as ref (ground) point.

17
Example #4 – Nodal Analysis
Find node voltages.

18
Example #5 – Nodal Analysis
Find node voltages.

19
Example #6 – Homework
Find node voltages.

20
Nodal Analysis with Voltage Sources
• Consider how voltage sources affect nodal analysis; two
possibilities:
• A voltage source is connected between the reference node and a
non-reference node:
• set the voltage at the non-reference node equal to the voltage of the
voltage source.
• A voltage source (dependent or independent) is connected
between two non-reference nodes:
• the two non-reference nodes (with the voltage source and any
elements connected in parallel with it) form a generalized node or
supernode
• apply both KCL and KVL to determine the node voltages.

21
Nodal Analysis with Voltage Sources

• First Case:
• v1 = 10V
• We know the voltage at this particular node.

• Second Case:
• A supernode is formed by enclosing a
(dependent or independent) voltage source
connected between two non-reference
nodes and any elements connected in
parallel with it.

22
Nodal Analysis with Voltage Sources

• KCL on supernode:
i1 + i4 = i2 + i3
v1 - v2 v1 - v3 v2 - 0 v3 - 0
+ = +
2 4 8 6
• KVL on supernode loop:

-v2 + 5 + v3 = 0
v2 - v3 = 5

23
Nodal Analysis with Voltage Sources

• The voltage source inside the supernode


provides a constraint equation needed to
solve for the node voltages.
• A supernode requires the application of both
KCL and KVL.

24
Example #7 – Nodal Analysis
Perform nodal analysis at v0

25
Example #8 – Nodal Analysis
Perform nodal analysis for v0

26
Example #9 – Nodal Analysis
Determine I. b

ref

27
Example #10 – Nodal Analysis
Find node voltages.

28
Example #10 – Nodal Analysis
Find node voltages.

29
Mesh Analysis
• Mesh analysis is another general procedure for analyzing circuits
• Uses mesh currents as the circuit variables
• Can reduce the number of simultaneous equations

• Loop and Mesh


• A loop is a closed path with no node passed more than once
• A mesh is a loop that does not contain any other loop within it

• Analysis types (so far):


• Nodal analysis applies KCL to find unknown voltages
• Mesh analysis applies KVL to find unknown currents

30
Mesh Analysis
• Concept:

31
Mesh Analysis
• Mesh analysis is not as general as nodal analysis.
• Only applies to a planar circuit
• A circuit that can be drawn in a plane with no
branches crossing one another.
• Otherwise it is nonplanar.
• A circuit may have crossing branches and still be
planar if it can be redrawn such that it has no
crossing branches.
• Circuit on right has two crossing branches, but it
can be redrawn so that is planar.

32
Mesh Analysis

• This circuit is nonplanar as there is no


way to redraw it and avoid the
branches crossing.
• Nonplanar circuits can be handled
using nodal analysis.

33
Mesh Analysis

1) Setup Circuit
• Assign mesh currents i1,i2,…,in to the n meshes
2) Setup Equations
• Apply KVL to each of the n meshes
• Use Ohm’s law to express voltages in terms of mesh currents
3) Solve the resulting simultaneous equations
• Solve to obtain the unknown mesh currents

34
Mesh Analysis – Step 1

• Mesh currents i1 and i2 are assigned


to meshes 1 and 2.
• The direction of mech current is
arbitrary (CW or CCW). Convention
to assume current is clockwise.
However, the direction does not
affect the validity of solution.
• Although path “abcdefa” is a loop and not a mesh, KVL still holds.
• This is the reason for loosely using the terms loop analysis and mesh
analysis to mean the same thing.
35
Mesh Analysis – Step 2

• Apply KVL at each mesh.


Mesh 1:
-V1+R1I1+R3I3=0
-V1+R1I1+R3(I1-I2)=0
(R1+R3)I1-R3I2=V1

Mesh 2:
𝐼! = 𝑖!, 𝐼" = 𝑖"
R2I2+V2-R3I3=0
R2I2+V2-R3(I1-I2)=0 𝐼# = 𝑖! − 𝑖"= 𝐼! − 𝐼"
-R3I1+(R2+R3)I2=-V2 36
Mesh Analysis – Step 3

• Solve the equations.


(R1+R3)I1-R3I2=V1
-R3I1+(R2+R3)I2=-V2

𝑅! + 𝑅" −𝑅" 𝐼! 𝑉!
=
−𝑅" 𝑅# + 𝑅" 𝐼# −𝑉#

I! = i! , I# = i# , I" = i! − i#

Notice that the branch currents can be different from the mesh currents
unless the mesh is isolated.
37
Example #11 – Mesh Analysis
How are v1 and v2 related?

38
Example #12 – Mesh Analysis
Find v1 and v2?

39
Example #13 – Mesh Analysis
Which circuit is planar?

40
Example #14 – Mesh Analysis
Which circuit is planar?

41
Example #15 – Mesh Analysis
Perform mesh analysis on the left loop.

42
Example #16 – Mesh Analysis
Perform mesh analysis on the right loop.

43
Example #17 – Homework
Find the currents through all branches.

Hint:

We know: I1+I2+I3=0

44
Example #18 – Mesh Analysis
Use mesh analysis to find Io.

45
Example #19 – Homework
Use nodal analysis to find Io and validate your
answer with Example #18.

Hint:
label all nodes
use branches current (and NOT mesh
currents)
Write KCL

46
Example #20 – Homework
Use mesh analysis to find Io.

Hint: write 3 KVL in 3 meshes and 1 KCL at


Node A.
Answer:
i1=2.25A
i2=0.75A
i3=1.5A
Io=1.5A

47
Mesh Analysis with Current Sources

• Applying mesh analysis to circuits


containing current sources is actually
much easier than previous methods.
• The current sources reduce the
number of equations.

• Example 21, First case:


• Current source is in only one i2 = -5A
mesh.
-10 + 4i1 + 6 ( i1 - i2 ) = 0
i1 = -2A
48
Mesh Analysis with Current Sources
• Second Case:
• A current source exists between two meshes
• Create a supermesh by excluding the current
source and any elements connected in series
with it.
• Example 22, KVL at the supermesh:
-20 + 6i1 + 10i2 + 4i2 = 0
6i1 + 14i2 = 20
• KCL to a node in the branch where the two
meshes interconnect, and solve:

i2 = i1 + 6
i1 = -3.2A i2 = 2.8A 49
Mesh Analysis with Current Sources

• The current source in the supermesh provides


the constraint equation necessary to solve for
the mesh currents.
• A supermesh requires the application of both
KVL and KCL.

50
Example #23 – Mesh Analysis
What is the equation for the supermesh?

51
Example #24 – Mesh Analysis
What is the constraining equation?

52
Example #23 & 24 – Mesh Analysis
Find currents of all elements.

53
Example #23 & 24 – Mesh Analysis
Find voltages of all elements.

54
Example #25 – Mesh Analysis
Find I0.

55
Example #26 – Mesh Analysis
Find v.

56
Example #27 – Mesh Analysis
Find V.

57
Example #28 – Mesh Analysis
Find V.

58
Example #29 – Homework
Use mesh analysis to find i1, i2, and i3.

59
Nodal Versus Mesh Analysis

Nodal Analysis Mesh Analysis


• Parallel-connected elements, • Series-connected elements,
current sources, or supernodes voltage sources, or supermeshes
• Fewer nodes than meshes • Fewer meshes than nodes
• Node voltages are required • Branch or mesh currents are
• Non-planar network required
• Computer solution • Transistor circuits

60
Nodal Versus Mesh Analysis

• Select the method that results in the smaller number of


equations.

• One method can be used to check the results from the other
method, if possible.

• Since each method has its limitations, only one method may
be suitable for a particular problem.

61

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