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BFF1303: ELECTRICAL / ELECTRONICS ENGINEERING Direct Current Circuits : Methods of Analysis Ismail Mohd Khairuddin , Zulkifil Md Yusof Faculty of Manufacturing Engineering Universiti Malaysia Pahang

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BFF1303: ELECTRICAL /

ELECTRONICS ENGINEERING

Direct Current Circuits :

Methods of Analysis

Ismail Mohd Khairuddin , Zulkifil Md Yusof

Faculty of Manufacturing Engineering Universiti Malaysia Pahang

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 2

Faculty of Manufacturing Universiti Malaysia Pahang

Kampus Pekan, Pahang Darul Makmur Tel: +609-424 5800 Fax: +609-4245888

Direct Current Circuit (DC)-

Methods of Analysis

BFF1303 ELECTRICAL/ELECTRONICS ENGINEERING

Contents:

Outcomes

Nodal Analysis

Mesh Analysis

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Compute the solution of circuits containing linear

resistors and independent and dependent sources by

using node analysis

Compute the solution of circuits containing linear

resistors and independent and dependent sources by

using mesh analysis

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There is another method to solve for currents and voltages. Easier

More methodical

Still based on Ohm’s Law, KVL and KCL

The methods are the nodal and mesh analysis.

Nodal analysis is based on the KCL.

Mesh analysis is based on the KVL.

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WITHOUT VOLTAGE SOURCE

Analyze the circuit using node voltages as the circuit variables.

The node voltages is chosen instead of the elements voltages.

To simplify matters, it is first assumed that the circuits do not contain voltage sources.

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i. Select a node as a reference node – This reference node also called the ground, have zero potential.

Steps to determine node voltages:

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ii. The other node (nonreference nodes) will be assigned as 𝑣1, 𝑣2, ⋯

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iii. Apply KCL to each of the nonreference node.

At node 𝑣1:

1 2 1 2I I i i

At node 𝑣2:

3 2 2i I i

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iv. Apply the Ohm’s law to express the unknown current 𝑖1, 𝑖2 and 𝑖3 in terms of node voltages.

higher lowerv vi

R

Note: Current flows from a higher potential (positive terminal) to a lower potential (negative terminal) in resistor.

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1 1 21 2

1 2

0v v vI I

R R

2 1 2

2

3 2

0v v vI

R R

11

1

0vi

R

1 2

2

2

v vi

R

23

3

0vi

R

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Obtain the node voltages for the following circuit

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Solution

i. Select a node as a reference node

ii. The other node (nonreference nodes) will be assigned as 𝑣1, 𝑣2 ⋯

iii. Apply KCL to each of the nonreference node.

At node 𝑣1:

1 2 3

1 2 3

0i i i

i i i

At node 𝑣2:

2 4 1 5

2 4 1 5

0i i i i

i i i i

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iv. Express the currents in term of node voltages.

1 2 154 2

v v v 1 2 210 5

4 6

v v v

1 22

4

v vi

1

3

0

2

vi

2

5

0

6

vi

Rearrange the equation

1 2

1 2

3 20

3 5 60

v v

v v

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Then in matrix form

1

2

3 1 20

3 5 60

v

v

By using Cramer’s Rule

3 115 3 12

3 5

11

20 1

60 5 100 6013.333V

12v

22

3 20

3 60 180 6020V

12v

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In the given circuit, obtain the node voltages

Answer

1 26V 42Vv v

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For the given circuit, determine the voltages at the nodes

Answer

1 2 34.8V 2.4V 2.4Vv v v

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i. Select a node as a reference node – This reference node also called the ground, have zero potential.

ii. The other node (nonreference nodes) will be assigned as 𝑣1, 𝑣2, ⋯

iii. Apply KCL to each of the nonreference node.

iv. Apply the Ohm’s law to express the unknown current 𝑖1, 𝑖2 and 𝑖3 in terms of node voltages.

higher lowerv vi

R

Review of steps for nodal analysis without voltage sources:

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WITH VOLTAGE SOURCE

Case 1

If a voltage source is connected between the reference node and a nonreference node. The voltage at the nonreference node equal to the voltage source.

1 10Vv

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Case 2

If the voltage source (dependent or independent) is connected between two nonreference nodes, the two nonreference nodes form a generalized node or supernode.

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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.

supernode

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A supernode requires the applications of both KCL and KVL.

A supernode has no voltage of its own.

A supernode can be assumed as one big node.

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i. Select a node as a reference node – This reference node also called the ground, have zero potential.

ii. Assign the other nodes (nonreference nodes) as 𝑣1, 𝑣2, ⋯ and identify the supernode.

iii. Apply KCL to each of the nonreference node and the supernode.

Steps for nodal analysis with voltage source:

Note: For supernode, apply the KCL around the supernode. Assume the supernode as one big node

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iv. Express the currents in term of node voltages.

higher lowerv vi

R

v. Apply KVL around the supernode.

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Obtain the node voltages for the following circuit

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Solution

i. Select a node as a reference node

ii. Assign the other node (nonreference nodes) as 𝑣1, 𝑣2 ⋯ and identify the supernode

iii. Apply KCL to each of the nonreference node and the supernode.

At node 𝑣1@1:

1

1

2 0

2A

i

i

At node 𝑣2@2:

2

2

7 0

7 A

i

i

At supernode 1 2

1 2

2 7 0

2 7

i i

i i

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iv. Express the currents in term of node voltages.

1 22 72 4

v v 1

1

0

2

vi

2

2

0

4

vi

Rearrange the equation

1 2

2 1

8 2 28

20 2

v v

v v

v. Apply KVL around the supernode.

1 2

2 1

2 0

2

v v

v v

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Then in matrix form

1

2

2 1 20

1 1 2

v

v

By using Cramer’s Rule

2 12 1 3

1 1

11

20 1

2 1 20 27.333V

3v

22

2 20

1 2 4 205.333V

3v

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Find 𝑣 and 𝑖 for the given circuit

Answer

400mV 2.8Av i

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Obtain the node voltages for the following circuit

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Solution

i. Select a node as a reference node

ii. Assign the other node (nonreference nodes) as 𝑣1, 𝑣2 ⋯ and identify the supernode

iii. Apply KCL to each of the nonreference node and the supernode.

At supernode 1-2:

3 1 2

3 1 2

10 0

10

i i i

i i i

At supernode 3-4: 1 3 4 5

1 3 4 5

0i i i i

i i i i

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iv. Express the currents in term of node voltages.

3 23

6

v vi

1 4

13

v vi

1

2

0

2

vi

44

0

1

vi

3

5

0

4

vi

3 2 1 4 1

1 2 3 4

106 3 2

5 2 60

v v v v v

v v v v

3 2 31 4 4

1 2 3 4

3 6 1 4

4 2 5 16 0

v v vv v v

v v v v

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v. Apply KVL around the supernode.

1 2

1 2

20 0

20

v v

v v

At loop 1

3 43 0xv v v

At loop 2

1 4xv v v and

1 3 43 2 0v v v

33 6 20 0x xv v i

At loop 3

1 4

3 3 26

xv v v

i v v

and

1 2 3 42 2 20v v v v

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From loop 1

2 1 20v v

and subs this Eq. into

1 2 3 45 2 60v v v v

1 2 3 44 2 5 16 0v v v v

and

1 3 46 2 80v v v

1 3 46 5 16 40v v v

Then in matrix form

1

3

4

3 1 2 0

6 1 2 80

6 5 16 40

v

v

v

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By using Cramer’s Rule

3 1 2

6 1 2 18

6 5 16

11

0 1 2

80 1 2

40 5 16 48026.667 V

18v

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33

3 0 2

6 80 2

6 40 16 3120173.333V

18v

44

3 1 0

6 1 80

6 5 40 84046.667 V

18v

2 1

2

20

26.667 20 6.667 V

v v

v

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By using nodal analysis obtain the node voltages for the following circuit

Answer

1 2 37.608V 17.39V 1.6305Vv v v

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WITHOUT CURRENT SOURCE

Mesh analysis use the mesh currents as the circuit variables.

Recall: nodal analysis use the node voltages as the circuit variables.

Recall: 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.

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Recall: nodal analysis applies KCL to find unknown voltages.

Mesh analysis applies KVL to find unknown currents.

abefa & bcdeb are meshes. abcdefa is not a mesh.

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The current through a mesh is known as mesh current.

First, the analysis will concentrate on circuit with no current source.

Steps to determine mesh currents: i. Assign mesh currents 𝑖1, 𝑖2, ⋯ , 𝑖𝑛 to the n meshes. The flow of the mesh

currents is conventionally assume in clockwise direction.

ii. Determine the polarity & the direction of current flow through each element.

iii. Apply KCL for each node in term of mesh current.

iv. Apply KVL to each of the n meshes. Use Ohm’s law to express the voltages in terms of the mesh currents.

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i. Assign the mesh currents: 𝑖1 and 𝑖2

ii. Determine the polarity & the direction of current.

Note: let the direction of current at the outside branch = direction of the mesh current

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iii. Apply KCL.

3 1 2I I I

Note: I for branch current, i for mesh current

since

1 1

2 2

I i

I i

3 1 2I i i

iv. Apply KVL to each mesh.

Mesh 1

1 1 2

1 2

15 5 10 10 0

3 2 1 1

i i i

i i

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Mesh 2

2 2 1 2

1 2

6 4 10 10 0

2 1 2

i i i i

i i

Then in matrix form

1

2

3 2 1

1 2 1

i

i

By using Cramer’s Rule

3 26 2 4

1 2

11

1 2

1 2 2 21A

4i

22

3 1

1 1 3 11A

3i

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Calculate the mesh current 𝑖1 and 𝑖2 for the following circuit

Answer

1 22.5A 0Ai i

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Use mesh analysis to find 𝐼𝑜 for the following circuit

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i. Assign the mesh currents: 𝑖1 and 𝑖2.

ii. Determine the polarity & the direction of current.

iii. Apply KCL.

1 2oI i i

iv. Apply KVL to each mesh.

Mesh 1

1 2 1 3

1 2 3

24 10 12 0

11 5 6 12 1

i i i i

i i i

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 46

Mesh 2

2 2 3 2 1

1 2 3

24 4 10 0

5 19 2 0 2

i i i i i

i i i

Mesh 3

1 2 3 1 3 2

1 2 3

4 12 4 0

2 0 3

i i i i i i

i i i

Then in matrix form

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 47

1

2

3

11 5 6 12

5 19 2 0

1 1 2 0

i

i

i

By using Cramer’s Rule

192

11

4322.25A

192i

22

1440.75A

192i

33

2881.5A

192i

Thus,

1 2 1.5AoI i i

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 48

By using mesh analysis find 𝐼𝑜 in the following circuit

Answer

4AoI

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BFF1303 Electrical/Electronic Engineering 49

WITH CURRENT SOURCE

Case 1

When the current source exist only in one mesh

Set the value of 𝑖2 = −5 A and write a mesh equation for the other mesh in the usual way.

1 1 2 110 4 6 0 2Ai i i i

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 50

Case 2

When the current source exist between two meshes.

need to create a supermesh by excluding the current source and any elements connected in series with it.

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 51

NOTE: A supermesh results when two meshes have a (dependent or independent) current source in common.

Applying KVL to the supermesh

1 2 2

1 2

20 6 10 4 0

6 14 20 1

i i i

i i

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 52

Applying KCL to the circuit

2 1 6 2i i

Then solve the Eq. (1) and (2) 1 23.2A 2.8Ai i

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 53

The current source in the supermesh provides the constraint equation necessary to solve for the mesh currents.

A supermesh has no current of its own.

A supermesh requires the application of both KVL and KCL.

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 54

By using mesh analysis find 𝑖1, 𝑖2 and 𝑖3 in the following circuit

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 55

i. Assign the mesh currents: 𝑖1, 𝑖2 and 𝑖3.

ii. Determine the polarity & the direction of current.

iii. Applying KCL to supermesh.

1 24 1i i

Notice that meshes (1) and (2) form a supermesh since they have independent current source in common

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BFF1303 Electrical/Electronic Engineering 56

iv. Apply KVL to supermesh.

1 3 2 3 2

1 2 3

8 2 4 8 0

2 12 6 8 2

i i i i i

i i i

Applying KVL in Mesh 3

3 3 2 3 1

1 2 3

2 4 2 0

2 4 8 0 3

i i i i i

i i i

Then in matrix form

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 57

1

2

3

1 1 0 4

2 12 6 8

2 4 8 0

i

i

i

By using Cramer’s Rule

76

11

3524.3516A

76i

22

480.6316A

76i

33

1121.4737 A

76i

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I Mohd-Khairuddin , Z Md-Yusof

BFF1303 Electrical/Electronic Engineering 58

By using mesh analysis find 𝑖1, to 𝑖4 in the following circuit

Answer

1 2 3 27.5A 2.5A 3.93A 2.143Ai i i i