ee -304 electrical network theory (loop/circuit matrix) [2016]
TRANSCRIPT
EE - 304 Electrical Network TheoryTie-Set(Loop) Matrix
North-Eastern Hill University
29.08.2016 joIp_rkas, ECE, NEHU, Shillong - 793 022
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Complete loop matrix or simply circuit matrix is used to describe the way in whichthe branches constitute loops or circuits in a graph.
- To write this matrix in a systematic way, an arbitrary orientation is specified foreach loop using an ordered list of its branches and nodes.
- The total number of loops are determined using an exhaustive search.
There are two types of loop/circuit matrices:- Complete loop/circuit matrix, BC,- Loop/circuit/tie-set matrix, B.
For a graph having n nodes and b branches, the complete loop matrix Bc , is arectangular matrix with b columns and as many rows as there are loops.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 1 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Complete loop matrix or simply circuit matrix is used to describe the way in whichthe branches constitute loops or circuits in a graph.
- To write this matrix in a systematic way, an arbitrary orientation is specified foreach loop using an ordered list of its branches and nodes.
- The total number of loops are determined using an exhaustive search.
There are two types of loop/circuit matrices:- Complete loop/circuit matrix, BC,- Loop/circuit/tie-set matrix, B.
For a graph having n nodes and b branches, the complete loop matrix Bc , is arectangular matrix with b columns and as many rows as there are loops.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 1 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Complete loop matrix or simply circuit matrix is used to describe the way in whichthe branches constitute loops or circuits in a graph.
- To write this matrix in a systematic way, an arbitrary orientation is specified foreach loop using an ordered list of its branches and nodes.
- The total number of loops are determined using an exhaustive search.
There are two types of loop/circuit matrices:- Complete loop/circuit matrix, BC,- Loop/circuit/tie-set matrix, B.
For a graph having n nodes and b branches, the complete loop matrix Bc , is arectangular matrix with b columns and as many rows as there are loops.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 1 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Complete loop matrix or simply circuit matrix is used to describe the way in whichthe branches constitute loops or circuits in a graph.
- To write this matrix in a systematic way, an arbitrary orientation is specified foreach loop using an ordered list of its branches and nodes.
- The total number of loops are determined using an exhaustive search.
There are two types of loop/circuit matrices:
- Complete loop/circuit matrix, BC,- Loop/circuit/tie-set matrix, B.
For a graph having n nodes and b branches, the complete loop matrix Bc , is arectangular matrix with b columns and as many rows as there are loops.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 1 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Complete loop matrix or simply circuit matrix is used to describe the way in whichthe branches constitute loops or circuits in a graph.
- To write this matrix in a systematic way, an arbitrary orientation is specified foreach loop using an ordered list of its branches and nodes.
- The total number of loops are determined using an exhaustive search.
There are two types of loop/circuit matrices:- Complete loop/circuit matrix, BC,
- Loop/circuit/tie-set matrix, B.
For a graph having n nodes and b branches, the complete loop matrix Bc , is arectangular matrix with b columns and as many rows as there are loops.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 1 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Complete loop matrix or simply circuit matrix is used to describe the way in whichthe branches constitute loops or circuits in a graph.
- To write this matrix in a systematic way, an arbitrary orientation is specified foreach loop using an ordered list of its branches and nodes.
- The total number of loops are determined using an exhaustive search.
There are two types of loop/circuit matrices:- Complete loop/circuit matrix, BC,- Loop/circuit/tie-set matrix, B.
For a graph having n nodes and b branches, the complete loop matrix Bc , is arectangular matrix with b columns and as many rows as there are loops.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 1 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Complete loop matrix or simply circuit matrix is used to describe the way in whichthe branches constitute loops or circuits in a graph.
- To write this matrix in a systematic way, an arbitrary orientation is specified foreach loop using an ordered list of its branches and nodes.
- The total number of loops are determined using an exhaustive search.
There are two types of loop/circuit matrices:- Complete loop/circuit matrix, BC,- Loop/circuit/tie-set matrix, B.
For a graph having n nodes and b branches, the complete loop matrix Bc , is arectangular matrix with b columns and as many rows as there are loops.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 1 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Circuits↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Loops↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
Orientation ofloops/circuits in the graphis considered to be arbitrary
while deriving Bc!
There will be b number ofcolumns in Bc!
Number of rows in Bcequals to that of possible
loops in the graph!
The elements of the complete loop/circuit matrix have the following values:
bij =
1, if the branch j is in the loop i and their orientations coincide,−1, if the branch j is in the loop i and their orientations are opposite,0, if the branch j is not in the loop i.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 2 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Circuits↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Loops↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
Orientation ofloops/circuits in the graphis considered to be arbitrary
while deriving Bc!
There will be b number ofcolumns in Bc!
Number of rows in Bcequals to that of possible
loops in the graph!
The elements of the complete loop/circuit matrix have the following values:
bij =
1, if the branch j is in the loop i and their orientations coincide,−1, if the branch j is in the loop i and their orientations are opposite,0, if the branch j is not in the loop i.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 2 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Circuits↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Loops↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
Orientation ofloops/circuits in the graphis considered to be arbitrary
while deriving Bc!
There will be b number ofcolumns in Bc!
Number of rows in Bcequals to that of possible
loops in the graph!
The elements of the complete loop/circuit matrix have the following values:
bij =
1, if the branch j is in the loop i and their orientations coincide,−1, if the branch j is in the loop i and their orientations are opposite,0, if the branch j is not in the loop i.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 2 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Circuits↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
That is, the complete loop matrix, Bc, of the graph of n nodes and b branches isBranches→
Loops↓ 1 2 3 4 . . . b
Bc =
L1L2L3L4L5L6...
b11 b12 b13 b14 . . . b1bb21 b22 b23 b24 . . . b2bb31 b32 b33 b34 . . . b3bb41 b42 b43 b44 . . . b4bb51 b52 b53 b54 . . . b5bb61 b62 b63 b64 . . . b6b...
......
......
...
Orientation ofloops/circuits in the graphis considered to be arbitrary
while deriving Bc!
There will be b number ofcolumns in Bc!
Number of rows in Bcequals to that of possible
loops in the graph!
The elements of the complete loop/circuit matrix have the following values:
bij =
1, if the branch j is in the loop i and their orientations coincide,−1, if the branch j is in the loop i and their orientations are opposite,0, if the branch j is not in the loop i.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 2 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix
25µF
25µF25µF
10 kΩ
10 kΩ10 kΩ
27 kΩ
27 kΩ27 kΩ
2 H
2 H2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix
25µF
25µF25µF
10 kΩ
10 kΩ10 kΩ
27 kΩ
27 kΩ27 kΩ
2 H
2 H2 H
ix
Check what’s missing in the given circuit!
- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix
25µF
25µF25µF
10 kΩ
10 kΩ10 kΩ
27 kΩ
27 kΩ27 kΩ
2 H
2 H2 H
ix
Check what’s missing in the given circuit!- Assign node numbers
- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!
a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodes
b. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
a
a
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix
25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
a
a
b
b cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
a
a
b
b c
c
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
a
a
b
b
c
c
d
d ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
a
a
b
b
c
c
d
d e
e ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
a
a
b
b
c
c
d
d
e
e f
f
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
a
a
b
b
c
c
d
d
e
e
f
f
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!
Or this way!!
1 2
34
ab
cd e
f
1
2 3
4
a
b
c
d
e f1
2 34
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f
1
2 3
4
a
b
c
d
e f
12 3
4
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Consider the following network and let’s find its Bc!
1 2 3
4
5 mA
5 mA
0.4ix
0.4ix25µF
25µF
25µF
10 kΩ
10 kΩ
10 kΩ
27 kΩ
27 kΩ
27 kΩ
2 H
2 H
2 H
ix
Check what’s missing in the given circuit!- Assign node numbers- Assign branch current directions
Let’s now draw the graph of the given circuit!a. Identify arbitrary locations for 4 nodesb. Connect nodes for each branch in order
1 2 3
4
aa
bb cc
dd ee ff
Graph could have been drawn this waydepending on the location of nodes!Or this way!!
1 2
34
ab
cd e
f1
2 3
4
a
b
c
d
e f
12 3
4
a
bc f
e
d
Or this way!
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 3 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
aa
bbcc
dd ee ff
a
b c
d e f
L2L4
L5L6L7
Loop 1: L1a,c,bLoop 2: L2b,e,dLoop 3: L3a,f,e,bLoop 4: L4a,c,e,dLoop 5: L5c,f,eLoop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2L3L4L5L6L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
b
c
c
d
d
e
e
f
f
a
b c
d e f
L2L4
L5L6L7
Loop 1: L1a,c,bLoop 2: L2b,e,dLoop 3: L3a,f,e,bLoop 4: L4a,c,e,dLoop 5: L5c,f,eLoop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2L3L4L5L6L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
b
c
c
d
d
e
e
f
f
a
b c
d e f
L2L4
L5L6L7
Loop 1: L1a,c,b
Loop 2: L2b,e,dLoop 3: L3a,f,e,bLoop 4: L4a,c,e,dLoop 5: L5c,f,eLoop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1
L2L3L4L5L6L7
1 -1 -1 0 0 0
0 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
bc
c
d
d
e
e f
f
a
b c
d e f
L2
L4L5L6
L7
Loop 1: L1a,c,b
Loop 2: L2b,e,d
Loop 3: L3a,f,e,bLoop 4: L4a,c,e,dLoop 5: L5c,f,eLoop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1
L2
L3L4L5L6L7
1 -1 -1 0 0 0
0 1 0 1 1 0
1 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
bc
c
d
d e
e
f
f
a
b c
d e f
L2L4
L5L6L7
Loop 1: L1a,c,bLoop 2: L2b,e,d
Loop 3: L3a,f,e,b
Loop 4: L4a,c,e,dLoop 5: L5c,f,eLoop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2
L3
L4L5L6L7
1 -1 -1 0 0 00 1 0 1 1 0
1 -1 0 0 -1 1
1 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
bc
c
d
d
e
e
ff
a
b c
d e f
L2
L4
L5L6L7
Loop 1: L1a,c,bLoop 2: L2b,e,dLoop 3: L3a,f,e,b
Loop 4: L4a,c,e,d
Loop 5: L5c,f,eLoop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2L3
L4
L5L6L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
1 0 -1 1 1 0
0 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
bc
c
d
d e
e
f
f
a
b c
d e f
L2L4
L5
L6L7
Loop 1: L1a,c,bLoop 2: L2b,e,dLoop 3: L3a,f,e,bLoop 4: L4a,c,e,d
Loop 5: L5c,f,e
Loop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2L3L4
L5
L6L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 0
0 0 1 0 -1 1
1 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
b
c
c
d
d e
e f
f
a
b c
d e f
L2L4
L5
L6
L7
Loop 1: L1a,c,bLoop 2: L2b,e,dLoop 3: L3a,f,e,bLoop 4: L4a,c,e,dLoop 5: L5c,f,e
Loop 6: L6a,f,d
Loop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2L3L4L5
L6
L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 1
1 0 0 1 0 1
0 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
a
a
b
b
c
c
d
d e
e f
f
a
b c
d e f
L2L4
L5L6
L7
Loop 1: L1a,c,bLoop 2: L2b,e,dLoop 3: L3a,f,e,bLoop 4: L4a,c,e,dLoop 5: L5c,f,eLoop 6: L6a,f,d
Loop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2L3L4L5L6
L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 1
0 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
Now, let’s find all possible loops on this graph below to get Bc.
1 2 3
4
a
b c
fed
Consider the clock-wise orientation for each loop, the complete loop matrix, Bc, is
1 2 3
4
aa
bbcc
dd ee ff
a
b c
d e f
L2L4
L5L6L7
Loop 1: L1a,c,bLoop 2: L2b,e,dLoop 3: L3a,f,e,bLoop 4: L4a,c,e,dLoop 5: L5c,f,eLoop 6: L6a,f,dLoop 7: L7b,c,f,d
In Bc, there will be: b branches −→ b columnsall loops −→ as many rows as loops the graph has
There are only 7 possible loops that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesLoops a b c d e f
Bc =
L1L2L3L4L5L6L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 4 / 14
Tie-Set (Loop/Circuit) MatrixComplete Loop/Circuit Matrix, Bc
1 2 3
4
a
b c
d e f
L2L4
L5L6L7
Consider the clock-wise orientation for each circuit, the complete circuit matrix, Bc, is
Circuit 1: L1a,c,bCircuit 2: L2b,e,dCircuit 3: L3a,f,e,bCircuit 4: L4a,c,e,dCircuit 5: L5c,f,eCircuit 6: L6a,f,dCircuit 7: L7b,c,f,d
There are only 7 possible circuits (closed paths) that can be drawn on the given graph!Thus, Bc has only 7 rows.
BranchesCircuits a b c d e f
Bc =
L1L2L3L4L5L6L7
1 -1 -1 0 0 00 1 0 1 1 01 -1 0 0 -1 11 0 -1 1 1 00 0 1 0 -1 11 0 0 1 0 10 1 1 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 5 / 14
Tie-Set (Loop/Circuit) Matrix, B
In a graph with n nodes and b branches, we know that there are t = n − 1 twigs in atree and l = b − t = b − n + 1 links in the co-tree.
Consider a tree of a graph:- Re-placement of each link one at a time in the tree forms a closed path or loop orcircuit. Thus, every link forms a unique loop, closed path or circuit called thefundamental loop (f-loop) or fundamental circuit (f-circuit) or tie-set, in short.
- The number of f-circuits is same as that of links in a given tree. Hence, thenumber of f -circuits or tie-sets is equal to l = b − n + 1.
- The reference direction of the f -loop is taken as that of the link.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 6 / 14
Tie-Set (Loop/Circuit) Matrix, B
In a graph with n nodes and b branches, we know that there are t = n − 1 twigs in atree and l = b − t = b − n + 1 links in the co-tree.
Consider a tree of a graph:- Re-placement of each link one at a time in the tree forms a closed path or loop orcircuit. Thus, every link forms a unique loop, closed path or circuit called thefundamental loop (f-loop) or fundamental circuit (f-circuit) or tie-set, in short.
- The number of f-circuits is same as that of links in a given tree. Hence, thenumber of f -circuits or tie-sets is equal to l = b − n + 1.
- The reference direction of the f -loop is taken as that of the link.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 6 / 14
Tie-Set (Loop/Circuit) Matrix, B
In a graph with n nodes and b branches, we know that there are t = n − 1 twigs in atree and l = b − t = b − n + 1 links in the co-tree.
Consider a tree of a graph:- Re-placement of each link one at a time in the tree forms a closed path or loop orcircuit. Thus, every link forms a unique loop, closed path or circuit called thefundamental loop (f-loop) or fundamental circuit (f-circuit) or tie-set, in short.
- The number of f-circuits is same as that of links in a given tree. Hence, thenumber of f -circuits or tie-sets is equal to l = b − n + 1.
- The reference direction of the f -loop is taken as that of the link.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 6 / 14
Tie-Set (Loop/Circuit) Matrix, B
In a graph with n nodes and b branches, we know that there are t = n − 1 twigs in atree and l = b − t = b − n + 1 links in the co-tree.
Consider a tree of a graph:- Re-placement of each link one at a time in the tree forms a closed path or loop orcircuit. Thus, every link forms a unique loop, closed path or circuit called thefundamental loop (f-loop) or fundamental circuit (f-circuit) or tie-set, in short.
- The number of f-circuits is same as that of links in a given tree. Hence, thenumber of f -circuits or tie-sets is equal to l = b − n + 1.
- The reference direction of the f -loop is taken as that of the link.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 6 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example: In the graph shown below, we select a tree:
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3f -loops/f -circuits/tie-sets are formed by
::::::::re-placing
:::::each
:::link
::::one
:::at
::a
::::time
:::in
:::the
:::::tree!
Possible tie-sets or f -loops or f -circuits are now given byf -circuits : L1a,b,c
: L2b,d,e: L3a,b,e,f
f -loops : L1a,b,c: L2b,d,e: L3a,b,e,f
tie-sets : L1a,b,c: L2b,d,e: L3a,b,e,f
Note: Orientation of f -loop/f -circuit/tie-set is that of the link.Note: Every link defines a fundamental loop/circuit/tie-set of the graph.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 7 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example: In the graph shown below, we select a tree: twigsa, b, e.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3f -loops/f -circuits/tie-sets are formed by
::::::::re-placing
:::::each
:::link
::::one
:::at
::a
::::time
:::in
:::the
:::::tree!
Possible tie-sets or f -loops or f -circuits are now given byf -circuits : L1a,b,c
: L2b,d,e: L3a,b,e,f
f -loops : L1a,b,c: L2b,d,e: L3a,b,e,f
tie-sets : L1a,b,c: L2b,d,e: L3a,b,e,f
Note: Orientation of f -loop/f -circuit/tie-set is that of the link.Note: Every link defines a fundamental loop/circuit/tie-set of the graph.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 7 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example: In the graph shown below, we select a tree: twigsa, b, e.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3f -loops/f -circuits/tie-sets are formed by
::::::::re-placing
:::::each
:::link
::::one
:::at
::a
::::time
:::in
:::the
:::::tree!
Possible tie-sets or f -loops or f -circuits are now given byf -circuits : L1a,b,c
: L2b,d,e: L3a,b,e,f
f -loops : L1a,b,c: L2b,d,e: L3a,b,e,f
tie-sets : L1a,b,c: L2b,d,e: L3a,b,e,f
Note: Orientation of f -loop/f -circuit/tie-set is that of the link.Note: Every link defines a fundamental loop/circuit/tie-set of the graph.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 7 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example: In the graph shown below, we select a tree: twigsa, b, e.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1
b
edL2
a
b
e f
L3
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
f -loops/f -circuits/tie-sets are formed by::::::::re-placing
:::::each
:::link
::::one
:::at
::a
::::time
:::in
:::the
:::::tree!
Possible tie-sets or f -loops or f -circuits are now given byf -circuits : L1a,b,c
: L2b,d,e: L3a,b,e,f
f -loops : L1a,b,c: L2b,d,e: L3a,b,e,f
tie-sets : L1a,b,c: L2b,d,e: L3a,b,e,f
Note: Orientation of f -loop/f -circuit/tie-set is that of the link.
Note: Every link defines a fundamental loop/circuit/tie-set of the graph.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 7 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example: In the graph shown below, we select a tree: twigsa, b, e.
1 2 3
4
a
b c
fed
1 2 3
4
a
b
c
f
ed
a
b c
L1
b
edL2
a
b
e f
L3
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
f -loops/f -circuits/tie-sets are formed by::::::::re-placing
:::::each
:::link
::::one
:::at
::a
::::time
:::in
:::the
:::::tree!
Possible tie-sets or f -loops or f -circuits are now given by
f -circuits : L1a,b,c: L2b,d,e: L3a,b,e,f
f -loops : L1a,b,c: L2b,d,e: L3a,b,e,f
tie-sets : L1a,b,c: L2b,d,e: L3a,b,e,f
Note: Orientation of f -loop/f -circuit/tie-set is that of the link.
Note: Every link defines a fundamental loop/circuit/tie-set of the graph.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 7 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example: In the graph shown below, we select a tree: twigsa, b, e.
1 2 3
4
a
b c
fed
1 2 3
4
a
b
c
fe
d
a
b c
L1b
edL2
a
b
e f
L3
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
f -loops/f -circuits/tie-sets are formed by::::::::re-placing
:::::each
:::link
::::one
:::at
::a
::::time
:::in
:::the
:::::tree!
Possible tie-sets or f -loops or f -circuits are now given by
f -circuits : L1a,b,c: L2b,d,e: L3a,b,e,f
f -loops : L1a,b,c: L2b,d,e: L3a,b,e,f
tie-sets : L1a,b,c: L2b,d,e: L3a,b,e,f
Note: Orientation of f -loop/f -circuit/tie-set is that of the link.
Note: Every link defines a fundamental loop/circuit/tie-set of the graph.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 7 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example: In the graph shown below, we select a tree: twigsa, b, e.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
f -loops/f -circuits/tie-sets are formed by::::::::re-placing
:::::each
:::link
::::one
:::at
::a
::::time
:::in
:::the
:::::tree!
Possible tie-sets or f -loops or f -circuits are now given by
f -circuits : L1a,b,c: L2b,d,e: L3a,b,e,f
f -loops : L1a,b,c: L2b,d,e: L3a,b,e,f
tie-sets : L1a,b,c: L2b,d,e: L3a,b,e,f
Note: Orientation of f -loop/f -circuit/tie-set is that of the link.
Note: Every link defines a fundamental loop/circuit/tie-set of the graph.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 7 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree:
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
f -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
Tie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f .
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
f -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
Tie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f . We now derive Tie-Set Matrix, B, by placing back each linkone at a time on the tree.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branchesf -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
Tie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f . We now derive Tie-Set Matrix, B, by placing back each linkone at a time on the tree.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1
b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 0
0 1 0 1 1 01 -1 0 0 -1 1
Branchesf -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
Tie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f . We now derive Tie-Set Matrix, B, by placing back each linkone at a time on the tree.
1 2 3
4
a
b c
fed
1 2 3
4
a
b
c
f
ed
a
b c
L1
b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 0
1 -1 0 0 -1 1
Branchesf -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
Tie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f . We now derive Tie-Set Matrix, B, by placing back each linkone at a time on the tree.
1 2 3
4
a
b c
fed
1 2 3
4
a
b
c
fe
d
a
b c
L1b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branchesf -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
Tie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f . We now derive Tie-Set Matrix, B, by placing back each linkone at a time on the tree.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branchesf -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
Tie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f . We now derive Tie-Set Matrix, B, by placing back each linkone at a time on the tree.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branchesf -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, BLet’s obtain the matrix!
Example - 1: In the graph shown below, we select a tree: twigsa, b, e. Thus, theco-tree: linksc, d , f . We now derive Tie-Set Matrix, B, by placing back each linkone at a time on the tree.
1 2 3
4
a
b c
fed
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
a
b
e f
L3
Tree : twigsa, b, e
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
a
b c
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
L3a, f , e, b
1 2 3
4
c
d
a
b
e f
L3
f -loops : L1a,b,c: L2b,e,d: L3a,f,e,b
f -circuits : L1a,b,c: L2b,e,d: L3a,f,e,b
tie-sets : L1a,b,c: L2b,e,d: L3a,f,e,b
Tie-Sets or f -Loops or f -Circuits are :
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
Branches
f -Circuits a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 -1 0 0 -1 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 8 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example - 2: We select a tree:
1 2 3
4
a
b c
fed
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3Tree : twigsa, b, d
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
Orientation ofloop/circuitchanges withthat of the link!
L3a, f , d
1 2 3
4
bc
e
a
fdL4
Tie-Sets or f -Loops or f -Circuits are : Tie-Set or f -Loop or f -Circuit matrix is :tie-sets : L1a,b,c
: L2b,e,d: L3a,f,d
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 0 0 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 9 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example - 2: We select a tree: twigsa, b, d. Thus, the co-tree: linksc, e, f .
1 2 3
4
a
b c
fed
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3Tree : twigsa, b, d
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
Orientation ofloop/circuitchanges withthat of the link!
L3a, f , d
1 2 3
4
bc
e
a
fdL4
Tie-Sets or f -Loops or f -Circuits are : Tie-Set or f -Loop or f -Circuit matrix is :tie-sets : L1a,b,c
: L2b,e,d: L3a,f,d
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 0 0 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 9 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example - 2: We select a tree: twigsa, b, d. Thus, the co-tree: linksc, e, f . Wenow derive Tie-Set Matrix, B, by placing back each link one at a time on the tree.
1 2 3
4
a
b c
fed
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
Tree : twigsa, b, d
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
Orientation ofloop/circuitchanges withthat of the link!
L3a, f , d
1 2 3
4
bc
e
a
fdL4
Tie-Sets or f -Loops or f -Circuits are : Tie-Set or f -Loop or f -Circuit matrix is :tie-sets : L1a,b,c
: L2b,e,d: L3a,f,d
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 0
0 1 0 1 1 01 0 0 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 9 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example - 2: We select a tree: twigsa, b, d. Thus, the co-tree: linksc, e, f . Wenow derive Tie-Set Matrix, B, by placing back each link one at a time on the tree.
1 2 3
4
a
b c
fed
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
Tree : twigsa, b, d
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
Orientation ofloop/circuitchanges withthat of the link!
L3a, f , d
1 2 3
4
bc
e
a
fdL4
Tie-Sets or f -Loops or f -Circuits are : Tie-Set or f -Loop or f -Circuit matrix is :tie-sets : L1a,b,c
: L2b,e,d: L3a,f,d
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 0
1 0 0 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 9 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example - 2: We select a tree: twigsa, b, d. Thus, the co-tree: linksc, e, f . Wenow derive Tie-Set Matrix, B, by placing back each link one at a time on the tree.
1 2 3
4
a
b c
fed
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
Tree : twigsa, b, d
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
Orientation ofloop/circuitchanges withthat of the link!
L3a, f , d
1 2 3
4
bc
e
a
fdL4
Tie-Sets or f -Loops or f -Circuits are : Tie-Set or f -Loop or f -Circuit matrix is :tie-sets : L1a,b,c
: L2b,e,d: L3a,f,d
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 0 0 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 9 / 14
Tie-Set (Loop/Circuit) Matrix, B
Example - 2: We select a tree: twigsa, b, d. Thus, the co-tree: linksc, e, f . Wenow derive Tie-Set Matrix, B, by placing back each link one at a time on the tree.
1 2 3
4
a
b c
fed
In the given diagram on the left, we haveNumber of nodes : n = 4
Number of branches : b = 6Number of branches on tree : t = n − 1 = 3
Number of links : l = b − t= b − (n − 1)= b − n + 1 = 3
Therefore, number of f -circuits : 3
Tree : twigsa, b, d
1 2 3
4
a
b c
fed
L1a, b, c
1 2 3
4
fed
a
b c
L1
L2b, e, d
1 2 3
4
a
c
f
b
edL2
Orientation ofloop/circuitchanges withthat of the link!
L3a, f , d
1 2 3
4
bc
e
a
fdL4
Tie-Sets or f -Loops or f -Circuits are : Tie-Set or f -Loop or f -Circuit matrix is :tie-sets : L1a,b,c
: L2b,e,d: L3a,f,d
BranchesTie-Sets a b c d e f
B =L1L2L3
-1 1 1 0 0 00 1 0 1 1 01 0 0 1 0 1
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 9 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree:
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
c
e fL3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :Branches
f -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f .
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
c
e fL3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :Branches
f -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f . We now derive Tie-Set Matrix, B, by placing backeach link one at a time on the tree.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
c
e fL3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :Branches
f -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f . We now derive Tie-Set Matrix, B, by placing backeach link one at a time on the tree.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
fed
a
b c
L1
b
edL2
c
e fL3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :Branches
f -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 0
0 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f . We now derive Tie-Set Matrix, B, by placing backeach link one at a time on the tree.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b
c
f
ed
a
b c
L1
b
edL2
c
e fL3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :Branches
f -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 0
0 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f . We now derive Tie-Set Matrix, B, by placing backeach link one at a time on the tree.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b
c
fe
d
a
b c
L1b
edL2
c
e fL3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :Branches
f -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f . We now derive Tie-Set Matrix, B, by placing backeach link one at a time on the tree.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
fed
a
b c
L1b
edL2
c
e fL3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :Branches
f -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f . We now derive Tie-Set Matrix, B, by placing backeach link one at a time on the tree.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
fed
a
b c
L1
b
ed
L2
c
e f
L3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set (Loop/Circuit) Matrix, BRank of the tie-set matrix!
Example - 3: In the graph shown below on the left, we select a tree: twigsb, c, e.Thus, the co-tree: linksa, d , f . We now derive Tie-Set Matrix, B, by placing backeach link one at a time on the tree.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
fed
a
b c
L1
b
ed
L2
c
e f
L3
f -loops : L1a,c,b: L2b,e,d: L3c,f,e
Tie-Sets or f -Loops or f -Circuits are :
Tie-Set or f -Loop or f -Circuit matrix is :
Branchesf -Loops a b c d e f
B =L1L2L3
1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
We now re-arrange columns in B with links first and twigs later as a, d , f , b, c, e.
Brancheslinks twigs
f -Loops a d f b c e
B =L1L2L3
1 0 0 -1 -1 00 1 0 1 0 10 0 1 0 1 -1
Thus, B = [Bl, Bt] = [I, Bt]. And B is non-singular matrix which rank is (b − n + 1).
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 10 / 14
Tie-Set Matrix, B, and KVL
Kirchhoff’s Voltage Law (KVL) of a graph can be applied to the f -loops to obtain aset of linearly independent equations.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
Tie-set 1 : Va − Vc − Vb=0Tie-set 2 : Vb + Ve + Vd=0Tie-set 3 : Vc + Vf − Ve=0
Expressing the above equations in matrix form as 1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
= 0
VaVbVcVdVeVf
Thus, BVB = 0 where VB is a column vector of branch voltages.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 11 / 14
Tie-Set Matrix, B, and KVL
Kirchhoff’s Voltage Law (KVL) of a graph can be applied to the f -loops to obtain aset of linearly independent equations. For this, we first select a tree as shown below.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
Tie-set 1 : Va − Vc − Vb=0Tie-set 2 : Vb + Ve + Vd=0Tie-set 3 : Vc + Vf − Ve=0
Expressing the above equations in matrix form as 1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
= 0
VaVbVcVdVeVf
Thus, BVB = 0 where VB is a column vector of branch voltages.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 11 / 14
Tie-Set Matrix, B, and KVL
Kirchhoff’s Voltage Law (KVL) of a graph can be applied to the f -loops to obtain aset of linearly independent equations. For this, we first select a tree as shown below.If Va, Vb, Vc , Vd , Ve and Vf are the branch voltages of branches a, b, c, d , e andf of the given graph, the KVL equation for each tie-set can be written as
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
Tie-set 1 : Va − Vc − Vb=0Tie-set 2 : Vb + Ve + Vd=0Tie-set 3 : Vc + Vf − Ve=0
Expressing the above equations in matrix form as 1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
= 0
VaVbVcVdVeVf
Thus, BVB = 0 where VB is a column vector of branch voltages.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 11 / 14
Tie-Set Matrix, B, and KVL
Kirchhoff’s Voltage Law (KVL) of a graph can be applied to the f -loops to obtain aset of linearly independent equations. For this, we first select a tree as shown below.If Va, Vb, Vc , Vd , Ve and Vf are the branch voltages of branches a, b, c, d , e andf of the given graph, the KVL equation for each tie-set can be written as
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
Tie-set 1 : Va − Vc − Vb=0Tie-set 2 : Vb + Ve + Vd=0Tie-set 3 : Vc + Vf − Ve=0
Expressing the above equations in matrix form as 1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
= 0
VaVbVcVdVeVf
Thus, BVB = 0 where VB is a column vector of branch voltages.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 11 / 14
Tie-Set Matrix, B, and KVL
Kirchhoff’s Voltage Law (KVL) of a graph can be applied to the f -loops to obtain aset of linearly independent equations. For this, we first select a tree as shown below.If Va, Vb, Vc , Vd , Ve and Vf are the branch voltages of branches a, b, c, d , e andf of the given graph, the KVL equation for each tie-set can be written as
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
Tie-set 1 : Va − Vc − Vb=0Tie-set 2 : Vb + Ve + Vd=0Tie-set 3 : Vc + Vf − Ve=0
Expressing the above equations in matrix form as 1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
= 0
VaVbVcVdVeVf
Thus, BVB = 0 where VB is a column vector of branch voltages.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 11 / 14
Tie-Set Matrix, B, and KVL
Kirchhoff’s Voltage Law (KVL) of a graph can be applied to the f -loops to obtain aset of linearly independent equations. For this, we first select a tree as shown below.If Va, Vb, Vc , Vd , Ve and Vf are the branch voltages of branches a, b, c, d , e andf of the given graph, the KVL equation for each tie-set can be written as
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
Tie-set 1 : Va − Vc − Vb=0Tie-set 2 : Vb + Ve + Vd=0Tie-set 3 : Vc + Vf − Ve=0
Expressing the above equations in matrix form as 1 -1 -1 0 0 00 1 0 1 1 00 0 1 0 -1 1
= 0
VaVbVcVdVeVf
Thus, BVB = 0 where VB is a column vector of branch voltages.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 11 / 14
Tie-Set Matrix, B, and Branch Currents
Branch currents can be expressed as a linear combination of link currents/loop cur-rents using B matrix as IB = B′IL where IB represents branch current matrix and ILthe loop current matrix.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
iaibicidieif
=
1 0 0−1 1 0−1 0 10 1 00 1 −10 0 1
IL1
IL2
IL3
Writing branch currents in terms of loop/link currents,ia = IL1
ib = −IL1 + IL2
ic = −IL1 + IL3
id = IL2
ie = IL2 − IL3
if = IL3
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 12 / 14
Tie-Set Matrix, B, and Branch Currents
Branch currents can be expressed as a linear combination of link currents/loop cur-rents using B matrix as IB = B′IL where IB represents branch current matrix and ILthe loop current matrix.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
iaibicidieif
=
1 0 0−1 1 0−1 0 10 1 00 1 −10 0 1
IL1
IL2
IL3
Writing branch currents in terms of loop/link currents,ia = IL1
ib = −IL1 + IL2
ic = −IL1 + IL3
id = IL2
ie = IL2 − IL3
if = IL3
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 12 / 14
Tie-Set Matrix, B, and Branch Currents
Branch currents can be expressed as a linear combination of link currents/loop cur-rents using B matrix as IB = B′IL where IB represents branch current matrix and ILthe loop current matrix.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
iaibicidieif
=
1 0 0−1 1 0−1 0 10 1 00 1 −10 0 1
IL1
IL2
IL3
Writing branch currents in terms of loop/link currents,ia = IL1
ib = −IL1 + IL2
ic = −IL1 + IL3
id = IL2
ie = IL2 − IL3
if = IL3
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 12 / 14
Tie-Set Matrix, B, and Branch Currents
Branch currents can be expressed as a linear combination of link currents/loop cur-rents using B matrix as IB = B′IL where IB represents branch current matrix and ILthe loop current matrix. i.e.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
iaibicidieif
=
1 0 0−1 1 0−1 0 10 1 00 1 −10 0 1
IL1
IL2
IL3
Writing branch currents in terms of loop/link currents,ia = IL1
ib = −IL1 + IL2
ic = −IL1 + IL3
id = IL2
ie = IL2 − IL3
if = IL3
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 12 / 14
Tie-Set Matrix, B, and Branch Currents
Branch currents can be expressed as a linear combination of link currents/loop cur-rents using B matrix as IB = B′IL where IB represents branch current matrix and ILthe loop current matrix. i.e.
1 2 3
4
a
b c
d e f
1 2 3
4
a
b c
d e f
Tree: twigsb, c, e
1 2 3
4
a
b c
d e f
Co-tree: linksa, d , f
1 2 3
4
a
b c
d e f
L1
L2 L3
iaibicidieif
=
1 0 0−1 1 0−1 0 10 1 00 1 −10 0 1
IL1
IL2
IL3
Writing branch currents in terms of loop/link currents,ia = IL1
ib = −IL1 + IL2
ic = −IL1 + IL3
id = IL2
ie = IL2 − IL3
if = IL3
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 12 / 14
Text Books & References
M. E. Van ValkenburgNetwork Analysis, 3/e.PHI, 2005.
W.H. Hayt, J.E. Kemmerly, S.M. DurbinEngineering Circuit Analysis, 8/e.MH, 2012.
D. Roy Choudhury,Networks and Systems,New Age Publishers, 1998.
M. Nahvi, J.A. EdministerSchuams Outline Electric Circuits, 4/e.TMH, SIE, 2007.
A. Sudhakar, S.S. PalliCircuits and Networks: Analysis and Synthesis, 2/e.TMH, 2002.
M. E. Van ValkenburgNetwork Analysis, 3/e.PHI, 2005.
W.H. Hayt, J.E. Kemmerly, S.M. DurbinEngineering Circuit Analysis, 8/e.MH, 2012.
D. Roy Choudhury,Networks and Systems,New Age Publishers, 1998.
M. Nahvi, J.A. EdministerSchuams Outline Electric Circuits, 4/e.TMH, SIE, 2007.
A. Sudhakar, S.S. PalliCircuits and Networks: Analysis and Synthesis, 2/e.TMH, 2002.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 13 / 14
Text Books & References
M. E. Van ValkenburgNetwork Analysis, 3/e.PHI, 2005.
W.H. Hayt, J.E. Kemmerly, S.M. DurbinEngineering Circuit Analysis, 8/e.MH, 2012.
D. Roy Choudhury,Networks and Systems,New Age Publishers, 1998.
M. Nahvi, J.A. EdministerSchuams Outline Electric Circuits, 4/e.TMH, SIE, 2007.
A. Sudhakar, S.S. PalliCircuits and Networks: Analysis and Synthesis, 2/e.TMH, 2002.
M. E. Van ValkenburgNetwork Analysis, 3/e.PHI, 2005.
W.H. Hayt, J.E. Kemmerly, S.M. DurbinEngineering Circuit Analysis, 8/e.MH, 2012.
D. Roy Choudhury,Networks and Systems,New Age Publishers, 1998.
M. Nahvi, J.A. EdministerSchuams Outline Electric Circuits, 4/e.TMH, SIE, 2007.
A. Sudhakar, S.S. PalliCircuits and Networks: Analysis and Synthesis, 2/e.TMH, 2002.
AeL. je. siHh/L. J. Singh(nehu/NEHU) EE - 304 Electrical Network Theory 29.08.2016 13 / 14