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Basic Electric Technology
Presented By:
Dr. Satish Kansal
Department of Electrical Engineering
BHSBIET Lehragaga
Outlines
 Loop-current
Analysis.
 Counting Independent
Loops.
 Mesh Analysis.
 Supermesh Method.
 Limitations of Mesh
Analysis.
 Planar Network.
 Procedure for Mesh
Analysis.
 Node Voltages
Analysis.
 Supernode.
 Counting Independent
Nodes.
 Nodal Analysis.
 Choice Between the
TWO.
3
 Loop analysis is systematic method of
network analysis.
 It is a general method and can be applied to
any electrical network, howsoever
complicated it may be.
 It is based on writing KVL equations for
independent loops.
 A loop is a closed path in a network.
 A node or a junction is a point in the network
where three or more elements have a
common connection.
Loop-current Analysis
4
 Before the loop analysis can be applied to a
network, we must first check that it has only
voltage sources (independent or dependent).
 Any current source must be transformed into
its equivalent voltage source.
 Sometimes, it is a difficult task to identify
independent loops in a network.
 The method of loop analysis can be best
understood by considering some examples.
5
Find the voltage across the 2-Ω resistance.
6
Recognize the independent loops (which does not pass
through a current source), and mark the loop currents.
This choice reduces labour, as only one current I1
is to be calculated.
7
Write KVL equations and solve for I1.
A0.435


1
1222
121
79)1)(()3()4(
67)2()1)((
I
IIII
III
9
•Suppose that we had marked the two loop
currents I1 and I2 in the standard way,
2 1 2AI I 
• The values of these two currents are
constrained by the above relation.
 India is in power deficient state
 power deficiency is nearly 12.2% of peak demand.
 In UP, MP, Maharashtra, Bihar, and Punjab; it is more than 20%.
 results in power cuts, blackouts, etc.
 The above mentioned causes make the Distribution Generation from
fuel cells, wind turbines, photovoltaic and small/micro hydro plants
for continuous growth of the country.
10
11
 We identify independent loops by turning
off all sources. We are, then, left with one
loop containing two resistances.
 Hence, we have only one independent
loop requiring only one KVL equation.
12
For determining the current through 5-Ω
resistance, we should choose
Thus, the single KVL equation is
A0.462

1
11 0)2(8510
I
II
13
In case, we are to determine the current through
8-Ω resistance, we should choose
The single KVL equation then becomes
A1.538

1
11 08)2(510
I
II
14
 In circuit terminology, a loop is any closed
path.
 A mesh is a special loop, namely, the
smallest loop one can have.
 In other words, a mesh is a loop that
contains no other loops.
 Mesh analysis is applicable only to a planar
network.
 However, most of the networks we shall need
to analyze are planar.
MESH ANALYSIS
15
 Once a circuit has been drawn in planar form,
it often looks like a multi-paned window.
 Each pane is a mesh.
 Meshes provide a set of independent
equations.
16
 If a network can be drawn on sheet of paper
without crossing lines, it is said to be planar.
• Yes, it is. Because it can be drawn in a
plane, as shown in the next figure.
17
• A planar network in which all branch currents
have been marked.
• While marking branch currents, we apply KCL at
each node to reduce the number of unknown
currents.
18
Is this a planar network ?
• This is definitely non-planar.
19
 By definition, a mesh-current is that current
which flows around the perimeter of a mesh.
It is indicated by a curved arrow that almost
closes on itself.
 Branch-currents have a physical identity. They
can be measured.
 Mesh-currents are fictitious.
 The mesh analysis not only tells us the
minimum number of unknown currents, but it
also ensures that the KVL equations obtained
are independent.
Mesh Currents

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Basic electric technology

  • 1. Basic Electric Technology Presented By: Dr. Satish Kansal Department of Electrical Engineering BHSBIET Lehragaga
  • 2. Outlines  Loop-current Analysis.  Counting Independent Loops.  Mesh Analysis.  Supermesh Method.  Limitations of Mesh Analysis.  Planar Network.  Procedure for Mesh Analysis.  Node Voltages Analysis.  Supernode.  Counting Independent Nodes.  Nodal Analysis.  Choice Between the TWO.
  • 3. 3  Loop analysis is systematic method of network analysis.  It is a general method and can be applied to any electrical network, howsoever complicated it may be.  It is based on writing KVL equations for independent loops.  A loop is a closed path in a network.  A node or a junction is a point in the network where three or more elements have a common connection. Loop-current Analysis
  • 4. 4  Before the loop analysis can be applied to a network, we must first check that it has only voltage sources (independent or dependent).  Any current source must be transformed into its equivalent voltage source.  Sometimes, it is a difficult task to identify independent loops in a network.  The method of loop analysis can be best understood by considering some examples.
  • 5. 5 Find the voltage across the 2-Ω resistance.
  • 6. 6 Recognize the independent loops (which does not pass through a current source), and mark the loop currents. This choice reduces labour, as only one current I1 is to be calculated.
  • 7. 7 Write KVL equations and solve for I1. A0.435   1 1222 121 79)1)(()3()4( 67)2()1)(( I IIII III
  • 8. 9 •Suppose that we had marked the two loop currents I1 and I2 in the standard way, 2 1 2AI I  • The values of these two currents are constrained by the above relation.
  • 9.  India is in power deficient state  power deficiency is nearly 12.2% of peak demand.  In UP, MP, Maharashtra, Bihar, and Punjab; it is more than 20%.  results in power cuts, blackouts, etc.  The above mentioned causes make the Distribution Generation from fuel cells, wind turbines, photovoltaic and small/micro hydro plants for continuous growth of the country. 10
  • 10. 11  We identify independent loops by turning off all sources. We are, then, left with one loop containing two resistances.  Hence, we have only one independent loop requiring only one KVL equation.
  • 11. 12 For determining the current through 5-Ω resistance, we should choose Thus, the single KVL equation is A0.462  1 11 0)2(8510 I II
  • 12. 13 In case, we are to determine the current through 8-Ω resistance, we should choose The single KVL equation then becomes A1.538  1 11 08)2(510 I II
  • 13. 14  In circuit terminology, a loop is any closed path.  A mesh is a special loop, namely, the smallest loop one can have.  In other words, a mesh is a loop that contains no other loops.  Mesh analysis is applicable only to a planar network.  However, most of the networks we shall need to analyze are planar. MESH ANALYSIS
  • 14. 15  Once a circuit has been drawn in planar form, it often looks like a multi-paned window.  Each pane is a mesh.  Meshes provide a set of independent equations.
  • 15. 16  If a network can be drawn on sheet of paper without crossing lines, it is said to be planar. • Yes, it is. Because it can be drawn in a plane, as shown in the next figure.
  • 16. 17 • A planar network in which all branch currents have been marked. • While marking branch currents, we apply KCL at each node to reduce the number of unknown currents.
  • 17. 18 Is this a planar network ? • This is definitely non-planar.
  • 18. 19  By definition, a mesh-current is that current which flows around the perimeter of a mesh. It is indicated by a curved arrow that almost closes on itself.  Branch-currents have a physical identity. They can be measured.  Mesh-currents are fictitious.  The mesh analysis not only tells us the minimum number of unknown currents, but it also ensures that the KVL equations obtained are independent. Mesh Currents