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Methods of Analysis Eastern Mediterranean University 1
Methods of
Analysis
Mustafa Kemal Uyguroğlu
Methods of Analysis
Eastern Mediterranean University
Methods of Analysis 2
• Introduction
• Nodal analysis
• Nodal analysis with voltage source
• Mesh analysis
• Mesh analysis with current source
• Nodal and mesh analyses by inspection
• Nodal versus mesh analysis
3.2 Nodal Analysis
Steps to Determine Node Voltages:
1. Select a node as the reference node. Assign voltage v1,
v2, …vn-1 to the remaining n-1 nodes. The voltages are
referenced with respect to the reference node.
2. Apply KCL to each of the n-1 nonreference nodes. Use
Ohm’s law to express the branch currents in terms of
node voltages.
3. Solve the resulting simultaneous equations to obtain
the unknown node voltages.
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Methods of Analysis 3
Figure 3.1
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Methods of Analysis 4
Common symbols for indicating a reference node,
(a) common ground, (b) ground, (c) chassis.
Figure 3.2
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Methods of Analysis 5
Typical circuit for nodal analysis
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Methods of Analysis 6
3
2
2
2
1
2
1
i
i
I
i
i
I
I





R
v
v
i lower
higher 

2
3
3
3
2
3
2
1
2
2
2
2
1
2
1
1
1
1
1
1
or
0
)
(
or
or
0
v
G
i
R
v
i
v
v
G
i
R
v
v
i
v
G
i
R
v
i










Eastern Mediterranean University
Methods of Analysis 7
3
2
2
2
1
2
2
2
1
1
1
2
1
R
v
R
v
v
I
R
v
v
R
v
I
I








2
3
2
1
2
2
2
1
2
1
1
2
1
)
(
)
(
v
G
v
v
G
I
v
v
G
v
G
I
I














 


















2
2
1
2
1
3
2
2
2
2
1
I
I
I
v
v
G
G
G
G
G
G
Example 3.1
Calculus the node voltage in the circuit shown in
Fig. 3.3(a)
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Methods of Analysis 8
Example 3.1
At node 1
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Methods of Analysis 9
2
0
4
5 1
2
1
3
2
1







v
v
v
i
i
i
Example 3.1
At node 2
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Methods of Analysis 10
6
0
4
5 2
1
2
5
1
4
2








v
v
v
i
i
i
i
Example 3.1
In matrix form:
Eastern Mediterranean University
Methods of Analysis 11



























5
5
4
1
6
1
4
1
4
1
4
1
2
1
2
1
v
v
Practice Problem 3.1
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Methods of Analysis 12
Fig 3.4
Example 3.2
Determine the voltage at the nodes in Fig. 3.5(a)
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Methods of Analysis 13
Example 3.2
At node 1,
Eastern Mediterranean University
Methods of Analysis 14
2
4
3
3
2
1
3
1
1
v
v
v
v
i
i x







Example 3.2
At node 2
Eastern Mediterranean University
Methods of Analysis 15
4
0
8
2
2
3
2
2
1
3
2








v
v
v
v
v
i
i
ix
Example 3.2
At node 3
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Methods of Analysis 16
2
)
(
2
8
4
2
2
1
3
2
3
1
2
1
v
v
v
v
v
v
i
i
i x








Example 3.2
In matrix form:
Eastern Mediterranean University
Methods of Analysis 17










































0
0
3
8
3
8
9
4
3
8
1
8
7
2
1
4
1
2
1
4
3
3
2
1
v
v
v
3.3 Nodal Analysis with Voltage Sources
Case 1: The voltage source is connected between a
nonreference node and the reference node: The
nonreference node voltage is equal to the
magnitude of voltage source and the number of
unknown nonreference nodes is reduced by one.
Case 2: The voltage source is connected between
two nonreferenced nodes: a generalized node
(supernode) is formed.
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Methods of Analysis 18
3.3 Nodal Analysis with Voltage Sources
5
6
0
8
0
4
2
3
2
3
2
3
1
2
1
3
2
4
1














v
v
v
v
v
v
v
v
i
i
i
i
Eastern Mediterranean University
Methods of Analysis 19
Fig. 3.7 A circuit with a supernode.
A supernode is formed by enclosing a (dependent
or independent) voltage source connected between
two nonreference nodes and any elements
connected in parallel with it.
The required two equations for regulating the two
nonreference node voltages are obtained by the
KCL of the supernode and the relationship of node
voltages due to the voltage source.
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Methods of Analysis 20
Example 3.3
For the circuit shown in Fig. 3.9, find the node
voltages.
2
0
4
2
7
2
0
2
1
7
2
2
1
2
1











v
v
v
v
i
i
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Methods of Analysis 21
i1 i2
Example 3.4
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Methods of Analysis 22
Find the node voltages in the circuit of Fig. 3.12.
Example 3.4
At suopernode 1-2,
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Methods of Analysis 23
20
2
3
10
6
2
1
1
4
1
2
3







v
v
v
v
v
v
v
Example 3.4
At supernode 3-4,
Eastern Mediterranean University
Methods of Analysis 24
)
(
3
4
1
6
3
4
1
4
3
3
4
2
3
4
1
v
v
v
v
v
v
v
v
v
v








3.4 Mesh Analysis
Mesh analysis: another procedure for analyzing
circuits, applicable to planar circuit.
A Mesh is a loop which does not contain any other
loops within it
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Methods of Analysis 25
Fig. 3.15
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Methods of Analysis 26
(a) A Planar circuit with crossing branches,
(b) The same circuit redrawn with no crossing branches.
Fig. 3.16
Eastern Mediterranean University
Methods of Analysis 27
A nonplanar circuit.
 Steps to Determine Mesh Currents:
1. Assign mesh currents i1, i2, .., in to the n meshes.
2. Apply KVL to each of the n meshes. Use Ohm’s law to
express the voltages in terms of the mesh currents.
3. Solve the resulting n simultaneous equations to get the
mesh currents.
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Methods of Analysis 28
Fig. 3.17
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Methods of Analysis 29
A circuit with two meshes.
Apply KVL to each mesh. For mesh 1,
For mesh 2,
Eastern Mediterranean University
Methods of Analysis 30
1
2
3
1
3
1
2
1
3
1
1
1
)
(
0
)
(
V
i
R
i
R
R
i
i
R
i
R
V








2
2
3
2
1
3
1
2
3
2
2
2
)
(
0
)
(
V
i
R
R
i
R
i
i
R
V
i
R









Solve for the mesh currents.
Use i for a mesh current and I for a branch current.
It’s evident from Fig. 3.17 that
Eastern Mediterranean University
Methods of Analysis 31
























2
1
2
1
3
2
3
3
3
1
V
V
i
i
R
R
R
R
R
R
2
1
3
2
2
1
1 ,
, i
i
I
i
I
i
I 



Example 3.5
Find the branch current I1, I2, and I3 using mesh
analysis.
Eastern Mediterranean University
Methods of Analysis 32
Example 3.5
For mesh 1,
For mesh 2,
We can find i1 and i2 by substitution method or
Cramer’s rule. Then,
Eastern Mediterranean University
Methods of Analysis 33
1
2
3
0
10
)
(
10
5
15
2
1
2
1
1








i
i
i
i
i
1
2
0
10
)
(
10
4
6
2
1
1
2
2
2







i
i
i
i
i
i
2
1
3
2
2
1
1 ,
, i
i
I
i
I
i
I 



Example 3.6
Use mesh analysis to find the current I0 in the
circuit of Fig. 3.20.
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Methods of Analysis 34
Example 3.6
Apply KVL to each mesh. For mesh 1,
For mesh 2,
Eastern Mediterranean University
Methods of Analysis 35
12
6
5
11
0
)
(
12
)
(
10
24
3
2
1
3
1
2
1









i
i
i
i
i
i
i
0
2
19
5
0
)
(
10
)
(
4
24
3
2
1
1
2
3
2
2









i
i
i
i
i
i
i
i
Example 3.6
For mesh 3,
In matrix from Eqs. (3.6.1) to (3.6.3) become
we can calculus i1, i2 and i3 by Cramer’s rule, and
find I0.
Eastern Mediterranean University
Methods of Analysis 36
0
2
0
)
(
4
)
(
12
)
(
4
,
A,
node
At
0
)
(
4
)
(
12
4
3
2
1
2
3
1
3
2
1
2
1
0
2
3
1
3
0

















i
i
i
i
i
i
i
i
i
i
I
I
i
i
i
i
I































0
0
12
2
1
1
2
19
5
6
5
11
3
2
1
i
i
i
3.5 Mesh Analysis with Current Sources
Eastern Mediterranean University
Methods of Analysis 37
Fig. 3.22 A circuit with a current source.
Case 1
● Current source exist only in one mesh
● One mesh variable is reduced
Case 2
● Current source exists between two meshes, a super-
mesh is obtained.
Eastern Mediterranean University
Methods of Analysis 38
A
2
1 

i
Fig. 3.23
a supermesh results when two meshes have a
(dependent , independent) current source in
common.
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Methods of Analysis 39
Properties of a Supermesh
1. The current is not completely ignored
● provides the constraint equation necessary to solve for
the mesh current.
2. A supermesh has no current of its own.
3. Several current sources in adjacency form a
bigger supermesh.
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Methods of Analysis 40
Example 3.7
For the circuit in Fig. 3.24, find i1 to i4 using mesh
analysis.
Eastern Mediterranean University
Methods of Analysis 41
 If a supermesh consists of two meshes, two
equations are needed; one is obtained using
KVL and Ohm’s law to the supermesh and the
other is obtained by relation regulated due to the
current source. 6
20
14
6
2
1
2
1





i
i
i
i
Eastern Mediterranean University
Methods of Analysis 42
Similarly, a supermesh formed from three meshes
needs three equations: one is from the supermesh
and the other two equations are obtained from the
two current sources.
Eastern Mediterranean University
Methods of Analysis 43
0
10
2
)
(
8
5
0
6
)
(
8
4
2
4
4
3
4
3
2
2
1
2
4
3
3
1















i
i
i
i
i
i
i
i
i
i
i
i
i
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Methods of Analysis 44
3.6 Nodal and Mesh Analysis by
Inspection
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Methods of Analysis 45
(a)For circuits with only resistors and
independent current sources
(b)For planar circuits with only resistors and
independent voltage sources
The analysis equations can be
obtained by direct inspection
In the Fig. 3.26 (a), the circuit has two
nonreference nodes and the node equations
Eastern Mediterranean University
Methods of Analysis 46





 

























2
2
1
2
1
3
2
2
2
2
1
2
3
2
1
2
2
2
1
2
1
1
2
1
)
8
.
3
(
)
(
)
7
.
3
(
)
(
I
I
I
v
v
G
G
G
G
G
G
MATRIX
v
G
v
v
G
I
v
v
G
v
G
I
I
In general, the node voltage equations in terms of
the conductances is
Eastern Mediterranean University
Methods of Analysis 47





































N
N
NN
N
N
N
N
i
i
i
v
v
v
G
G
G
G
G
G
G
G
G









2
1
2
1
2
1
2
22
21
1
12
11
or simply
Gv = i
where G : the conductance matrix,
v : the output vector, i : the input vector
The circuit has two nonreference nodes and the
node equations were derived as
Eastern Mediterranean University
Methods of Analysis 48
























2
1
2
1
3
2
3
3
3
1
v
v
i
i
R
R
R
R
R
R
In general, if the circuit has N meshes, the mesh-
current equations as the resistances term is
Eastern Mediterranean University
Methods of Analysis 49





































N
N
NN
N
N
N
N
v
v
v
i
i
i
R
R
R
R
R
R
R
R
R









2
1
2
1
2
1
2
22
21
1
12
11
or simply
Rv = i
where R : the resistance matrix,
i : the output vector, v : the input vector
Example 3.8
Write the node voltage matrix equations in Fig.3.27.
Eastern Mediterranean University
Methods of Analysis 50
Example 3.8
The circuit has 4 nonreference nodes, so
The off-diagonal terms are
Eastern Mediterranean University
Methods of Analysis 51
625
.
1
1
1
2
1
8
1
,
5
.
0
4
1
8
1
8
1
325
.
1
1
1
8
1
5
1
,
3
.
0
10
1
5
1
44
33
22
11















G
G
G
G
125
.
0
,
1
,
0
125
.
0
,
125
.
0
,
0
1
1
1
,
125
.
0
8
1
,
2
.
0
0
,
2
.
0
5
1
43
42
41
34
32
31
24
23
21
14
13
12


























G
G
G
G
G
G
G
G
G
G
G
G
Example 3.8
The input current vector i in amperes
The node-voltage equations are
Eastern Mediterranean University
Methods of Analysis 52
6
4
2
,
0
,
3
2
1
,
3 4
3
2
1 








 i
i
i
i














































6
0
3
3
.625
1
0.125
1
0
0.125
.5
0
0.125
0
1
0.125
.325
1
0.2
0
0
0.2
.3
0
4
3
2
1
v
v
v
v
Example 3.9
Write the mesh current equations in Fig.3.27.
Eastern Mediterranean University
Methods of Analysis 53
Example 3.9
The input voltage vector v in volts
The mesh-current equations are
Eastern Mediterranean University
Methods of Analysis 54
6
,
0
,
6
6
12
,
6
4
10
,
4
5
4
3
2
1












v
v
v
v
v












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













































6
0
6
6
4
4
3
0
1
0
3
8
0
1
0
0
0
9
4
2
1
1
4
0
1
2
0
0
2
2
9
5
4
3
2
1
i
i
i
i
i
3.7 Nodal Versus Mesh Analysis
Both nodal and mesh analyses provide a systematic
way of analyzing a complex network.
The choice of the better method dictated by two
factors.
● First factor : nature of the particular network. The key
is to select the method that results in the smaller
number of equations.
● Second factor : information required.
Eastern Mediterranean University
Methods of Analysis 55
BJT Circuit Models
Eastern Mediterranean University
Methods of Analysis 56
(a)An npn transistor,
(b) dc equivalent model.
Example 3.13
For the BJT circuit in Fig.3.43, =150 and VBE =
0.7 V. Find v0.
Eastern Mediterranean University
Methods of Analysis 57
Example 3.13
Use mesh analysis or nodal analysis
Eastern Mediterranean University
Methods of Analysis 58
Example 3.13
Eastern Mediterranean University
Methods of Analysis 59
3.10 Summery
1. Nodal analysis: the application of KCL at the
nonreference nodes
● A circuit has fewer node equations
2. A supernode: two nonreference nodes
3. Mesh analysis: the application of KVL
● A circuit has fewer mesh equations
4. A supermesh: two meshes
Eastern Mediterranean University
Methods of Analysis 60
Homework
Problems 7, 12, 20, 31(write down required
equations only), 39, 49, 53(write down required
equations only)
Eastern Mediterranean University
Methods of Analysis 61

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chap3.ppt

  • 1. Methods of Analysis Eastern Mediterranean University 1 Methods of Analysis Mustafa Kemal Uyguroğlu
  • 2. Methods of Analysis Eastern Mediterranean University Methods of Analysis 2 • Introduction • Nodal analysis • Nodal analysis with voltage source • Mesh analysis • Mesh analysis with current source • Nodal and mesh analyses by inspection • Nodal versus mesh analysis
  • 3. 3.2 Nodal Analysis Steps to Determine Node Voltages: 1. Select a node as the reference node. Assign voltage v1, v2, …vn-1 to the remaining n-1 nodes. The voltages are referenced with respect to the reference node. 2. Apply KCL to each of the n-1 nonreference nodes. Use Ohm’s law to express the branch currents in terms of node voltages. 3. Solve the resulting simultaneous equations to obtain the unknown node voltages. Eastern Mediterranean University Methods of Analysis 3
  • 4. Figure 3.1 Eastern Mediterranean University Methods of Analysis 4 Common symbols for indicating a reference node, (a) common ground, (b) ground, (c) chassis.
  • 5. Figure 3.2 Eastern Mediterranean University Methods of Analysis 5 Typical circuit for nodal analysis
  • 6. Eastern Mediterranean University Methods of Analysis 6 3 2 2 2 1 2 1 i i I i i I I      R v v i lower higher   2 3 3 3 2 3 2 1 2 2 2 2 1 2 1 1 1 1 1 1 or 0 ) ( or or 0 v G i R v i v v G i R v v i v G i R v i          
  • 7. Eastern Mediterranean University Methods of Analysis 7 3 2 2 2 1 2 2 2 1 1 1 2 1 R v R v v I R v v R v I I         2 3 2 1 2 2 2 1 2 1 1 2 1 ) ( ) ( v G v v G I v v G v G I I                                   2 2 1 2 1 3 2 2 2 2 1 I I I v v G G G G G G
  • 8. Example 3.1 Calculus the node voltage in the circuit shown in Fig. 3.3(a) Eastern Mediterranean University Methods of Analysis 8
  • 9. Example 3.1 At node 1 Eastern Mediterranean University Methods of Analysis 9 2 0 4 5 1 2 1 3 2 1        v v v i i i
  • 10. Example 3.1 At node 2 Eastern Mediterranean University Methods of Analysis 10 6 0 4 5 2 1 2 5 1 4 2         v v v i i i i
  • 11. Example 3.1 In matrix form: Eastern Mediterranean University Methods of Analysis 11                            5 5 4 1 6 1 4 1 4 1 4 1 2 1 2 1 v v
  • 12. Practice Problem 3.1 Eastern Mediterranean University Methods of Analysis 12 Fig 3.4
  • 13. Example 3.2 Determine the voltage at the nodes in Fig. 3.5(a) Eastern Mediterranean University Methods of Analysis 13
  • 14. Example 3.2 At node 1, Eastern Mediterranean University Methods of Analysis 14 2 4 3 3 2 1 3 1 1 v v v v i i x       
  • 15. Example 3.2 At node 2 Eastern Mediterranean University Methods of Analysis 15 4 0 8 2 2 3 2 2 1 3 2         v v v v v i i ix
  • 16. Example 3.2 At node 3 Eastern Mediterranean University Methods of Analysis 16 2 ) ( 2 8 4 2 2 1 3 2 3 1 2 1 v v v v v v i i i x        
  • 17. Example 3.2 In matrix form: Eastern Mediterranean University Methods of Analysis 17                                           0 0 3 8 3 8 9 4 3 8 1 8 7 2 1 4 1 2 1 4 3 3 2 1 v v v
  • 18. 3.3 Nodal Analysis with Voltage Sources Case 1: The voltage source is connected between a nonreference node and the reference node: The nonreference node voltage is equal to the magnitude of voltage source and the number of unknown nonreference nodes is reduced by one. Case 2: The voltage source is connected between two nonreferenced nodes: a generalized node (supernode) is formed. Eastern Mediterranean University Methods of Analysis 18
  • 19. 3.3 Nodal Analysis with Voltage Sources 5 6 0 8 0 4 2 3 2 3 2 3 1 2 1 3 2 4 1               v v v v v v v v i i i i Eastern Mediterranean University Methods of Analysis 19 Fig. 3.7 A circuit with a supernode.
  • 20. A supernode is formed by enclosing a (dependent or independent) voltage source connected between two nonreference nodes and any elements connected in parallel with it. The required two equations for regulating the two nonreference node voltages are obtained by the KCL of the supernode and the relationship of node voltages due to the voltage source. Eastern Mediterranean University Methods of Analysis 20
  • 21. Example 3.3 For the circuit shown in Fig. 3.9, find the node voltages. 2 0 4 2 7 2 0 2 1 7 2 2 1 2 1            v v v v i i Eastern Mediterranean University Methods of Analysis 21 i1 i2
  • 22. Example 3.4 Eastern Mediterranean University Methods of Analysis 22 Find the node voltages in the circuit of Fig. 3.12.
  • 23. Example 3.4 At suopernode 1-2, Eastern Mediterranean University Methods of Analysis 23 20 2 3 10 6 2 1 1 4 1 2 3        v v v v v v v
  • 24. Example 3.4 At supernode 3-4, Eastern Mediterranean University Methods of Analysis 24 ) ( 3 4 1 6 3 4 1 4 3 3 4 2 3 4 1 v v v v v v v v v v        
  • 25. 3.4 Mesh Analysis Mesh analysis: another procedure for analyzing circuits, applicable to planar circuit. A Mesh is a loop which does not contain any other loops within it Eastern Mediterranean University Methods of Analysis 25
  • 26. Fig. 3.15 Eastern Mediterranean University Methods of Analysis 26 (a) A Planar circuit with crossing branches, (b) The same circuit redrawn with no crossing branches.
  • 27. Fig. 3.16 Eastern Mediterranean University Methods of Analysis 27 A nonplanar circuit.
  • 28.  Steps to Determine Mesh Currents: 1. Assign mesh currents i1, i2, .., in to the n meshes. 2. Apply KVL to each of the n meshes. Use Ohm’s law to express the voltages in terms of the mesh currents. 3. Solve the resulting n simultaneous equations to get the mesh currents. Eastern Mediterranean University Methods of Analysis 28
  • 29. Fig. 3.17 Eastern Mediterranean University Methods of Analysis 29 A circuit with two meshes.
  • 30. Apply KVL to each mesh. For mesh 1, For mesh 2, Eastern Mediterranean University Methods of Analysis 30 1 2 3 1 3 1 2 1 3 1 1 1 ) ( 0 ) ( V i R i R R i i R i R V         2 2 3 2 1 3 1 2 3 2 2 2 ) ( 0 ) ( V i R R i R i i R V i R         
  • 31. Solve for the mesh currents. Use i for a mesh current and I for a branch current. It’s evident from Fig. 3.17 that Eastern Mediterranean University Methods of Analysis 31                         2 1 2 1 3 2 3 3 3 1 V V i i R R R R R R 2 1 3 2 2 1 1 , , i i I i I i I    
  • 32. Example 3.5 Find the branch current I1, I2, and I3 using mesh analysis. Eastern Mediterranean University Methods of Analysis 32
  • 33. Example 3.5 For mesh 1, For mesh 2, We can find i1 and i2 by substitution method or Cramer’s rule. Then, Eastern Mediterranean University Methods of Analysis 33 1 2 3 0 10 ) ( 10 5 15 2 1 2 1 1         i i i i i 1 2 0 10 ) ( 10 4 6 2 1 1 2 2 2        i i i i i i 2 1 3 2 2 1 1 , , i i I i I i I    
  • 34. Example 3.6 Use mesh analysis to find the current I0 in the circuit of Fig. 3.20. Eastern Mediterranean University Methods of Analysis 34
  • 35. Example 3.6 Apply KVL to each mesh. For mesh 1, For mesh 2, Eastern Mediterranean University Methods of Analysis 35 12 6 5 11 0 ) ( 12 ) ( 10 24 3 2 1 3 1 2 1          i i i i i i i 0 2 19 5 0 ) ( 10 ) ( 4 24 3 2 1 1 2 3 2 2          i i i i i i i i
  • 36. Example 3.6 For mesh 3, In matrix from Eqs. (3.6.1) to (3.6.3) become we can calculus i1, i2 and i3 by Cramer’s rule, and find I0. Eastern Mediterranean University Methods of Analysis 36 0 2 0 ) ( 4 ) ( 12 ) ( 4 , A, node At 0 ) ( 4 ) ( 12 4 3 2 1 2 3 1 3 2 1 2 1 0 2 3 1 3 0                  i i i i i i i i i i I I i i i i I                                0 0 12 2 1 1 2 19 5 6 5 11 3 2 1 i i i
  • 37. 3.5 Mesh Analysis with Current Sources Eastern Mediterranean University Methods of Analysis 37 Fig. 3.22 A circuit with a current source.
  • 38. Case 1 ● Current source exist only in one mesh ● One mesh variable is reduced Case 2 ● Current source exists between two meshes, a super- mesh is obtained. Eastern Mediterranean University Methods of Analysis 38 A 2 1   i
  • 39. Fig. 3.23 a supermesh results when two meshes have a (dependent , independent) current source in common. Eastern Mediterranean University Methods of Analysis 39
  • 40. Properties of a Supermesh 1. The current is not completely ignored ● provides the constraint equation necessary to solve for the mesh current. 2. A supermesh has no current of its own. 3. Several current sources in adjacency form a bigger supermesh. Eastern Mediterranean University Methods of Analysis 40
  • 41. Example 3.7 For the circuit in Fig. 3.24, find i1 to i4 using mesh analysis. Eastern Mediterranean University Methods of Analysis 41
  • 42.  If a supermesh consists of two meshes, two equations are needed; one is obtained using KVL and Ohm’s law to the supermesh and the other is obtained by relation regulated due to the current source. 6 20 14 6 2 1 2 1      i i i i Eastern Mediterranean University Methods of Analysis 42
  • 43. Similarly, a supermesh formed from three meshes needs three equations: one is from the supermesh and the other two equations are obtained from the two current sources. Eastern Mediterranean University Methods of Analysis 43
  • 45. 3.6 Nodal and Mesh Analysis by Inspection Eastern Mediterranean University Methods of Analysis 45 (a)For circuits with only resistors and independent current sources (b)For planar circuits with only resistors and independent voltage sources The analysis equations can be obtained by direct inspection
  • 46. In the Fig. 3.26 (a), the circuit has two nonreference nodes and the node equations Eastern Mediterranean University Methods of Analysis 46                                 2 2 1 2 1 3 2 2 2 2 1 2 3 2 1 2 2 2 1 2 1 1 2 1 ) 8 . 3 ( ) ( ) 7 . 3 ( ) ( I I I v v G G G G G G MATRIX v G v v G I v v G v G I I
  • 47. In general, the node voltage equations in terms of the conductances is Eastern Mediterranean University Methods of Analysis 47                                      N N NN N N N N i i i v v v G G G G G G G G G          2 1 2 1 2 1 2 22 21 1 12 11 or simply Gv = i where G : the conductance matrix, v : the output vector, i : the input vector
  • 48. The circuit has two nonreference nodes and the node equations were derived as Eastern Mediterranean University Methods of Analysis 48                         2 1 2 1 3 2 3 3 3 1 v v i i R R R R R R
  • 49. In general, if the circuit has N meshes, the mesh- current equations as the resistances term is Eastern Mediterranean University Methods of Analysis 49                                      N N NN N N N N v v v i i i R R R R R R R R R          2 1 2 1 2 1 2 22 21 1 12 11 or simply Rv = i where R : the resistance matrix, i : the output vector, v : the input vector
  • 50. Example 3.8 Write the node voltage matrix equations in Fig.3.27. Eastern Mediterranean University Methods of Analysis 50
  • 51. Example 3.8 The circuit has 4 nonreference nodes, so The off-diagonal terms are Eastern Mediterranean University Methods of Analysis 51 625 . 1 1 1 2 1 8 1 , 5 . 0 4 1 8 1 8 1 325 . 1 1 1 8 1 5 1 , 3 . 0 10 1 5 1 44 33 22 11                G G G G 125 . 0 , 1 , 0 125 . 0 , 125 . 0 , 0 1 1 1 , 125 . 0 8 1 , 2 . 0 0 , 2 . 0 5 1 43 42 41 34 32 31 24 23 21 14 13 12                           G G G G G G G G G G G G
  • 52. Example 3.8 The input current vector i in amperes The node-voltage equations are Eastern Mediterranean University Methods of Analysis 52 6 4 2 , 0 , 3 2 1 , 3 4 3 2 1           i i i i                                               6 0 3 3 .625 1 0.125 1 0 0.125 .5 0 0.125 0 1 0.125 .325 1 0.2 0 0 0.2 .3 0 4 3 2 1 v v v v
  • 53. Example 3.9 Write the mesh current equations in Fig.3.27. Eastern Mediterranean University Methods of Analysis 53
  • 54. Example 3.9 The input voltage vector v in volts The mesh-current equations are Eastern Mediterranean University Methods of Analysis 54 6 , 0 , 6 6 12 , 6 4 10 , 4 5 4 3 2 1             v v v v v                                                            6 0 6 6 4 4 3 0 1 0 3 8 0 1 0 0 0 9 4 2 1 1 4 0 1 2 0 0 2 2 9 5 4 3 2 1 i i i i i
  • 55. 3.7 Nodal Versus Mesh Analysis Both nodal and mesh analyses provide a systematic way of analyzing a complex network. The choice of the better method dictated by two factors. ● First factor : nature of the particular network. The key is to select the method that results in the smaller number of equations. ● Second factor : information required. Eastern Mediterranean University Methods of Analysis 55
  • 56. BJT Circuit Models Eastern Mediterranean University Methods of Analysis 56 (a)An npn transistor, (b) dc equivalent model.
  • 57. Example 3.13 For the BJT circuit in Fig.3.43, =150 and VBE = 0.7 V. Find v0. Eastern Mediterranean University Methods of Analysis 57
  • 58. Example 3.13 Use mesh analysis or nodal analysis Eastern Mediterranean University Methods of Analysis 58
  • 59. Example 3.13 Eastern Mediterranean University Methods of Analysis 59
  • 60. 3.10 Summery 1. Nodal analysis: the application of KCL at the nonreference nodes ● A circuit has fewer node equations 2. A supernode: two nonreference nodes 3. Mesh analysis: the application of KVL ● A circuit has fewer mesh equations 4. A supermesh: two meshes Eastern Mediterranean University Methods of Analysis 60
  • 61. Homework Problems 7, 12, 20, 31(write down required equations only), 39, 49, 53(write down required equations only) Eastern Mediterranean University Methods of Analysis 61