Course Name: Network Theory (PCCET303T)
Course In-charge: MOHAMMAD WASEEM AKRAM
Course Seminar on
“Norton’s Theorem”
Presented by
✽ 28 CHAITALI UKE ✽ 29 CHAITALI INGALE
Edward Lawry Norton
Norton’s Theorem
Statement:
Any linear bilateral complicated circuit with multiple
energy source and resistance can be replaced by a constant
current source in parallel with a resistor connected across
the load.
IN ➳ The short-circuit current through the terminals
RN ➳ Input/Equivalent resistance at the terminals when the independent source are
turned off
➺
Norton's equivalent
circuit
Steps to Solve Norton’s Theorem
01 02
04
05
03
Identify the load resistance RL
and short the load terminal of the
circuit.
By utilizing any network
simplification technique, determine the
current flowing through the shorted
branch. This current will be the Norton’s
current, IN.
Now remove RL from the give
circuit and replace all the active
sources with their equivalent
internal resistance.
Further, evaluate the equivalent
resistance across the open ends of the
circuit. This resistance will be the
Norton’s equivalent resistance RN.
Now, draw Norton's equivalent
circuit, comprising of IN in parallel
combination with RN across the load
resistance RL. Then find the current
through the load resistance RL using:
Consider the circuit showm below:
Numerical Implementation of Norton’s Theorem
➠
IN
↻
i1 i2 i3
For mesh 1,
50 = 5 i1 + 5 (i1 - i2 )
50 = 10 i1 - 5 i2
For mesh 2,
0 = 10 i2 + 5 (i2 – i1 ) + 5 (i2 – i3 )
0 = 5i1 - 20 i2 - 5 i3
For mesh 3,
0 = 5 (i3 – i2 )
i2 = i3 = N = 2A
For calculating RN:
Numerical Implementation of Norton’s Theorem
➠ RN
RN = {( 5 II 5 ) + 10} II 5
RN = {(
5∗5
5+5
) + 10} II 5
RN = {( 2.5) + 10} II 5
RN = ( 12.5) II 5
RN = (
12.5∗5
12.5+5
)
RN = 3.5 Ω
Numerical Implementation of Norton’s Theorem
Norton's Equivalent Circuit:
IL
= NRN
RN+RL
=
2 ∗ 3.5
2 + 3.5
= 1.27A
THANK YOU
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NT PPT[Norton’s Theorem].pdf

  • 1.
    Course Name: NetworkTheory (PCCET303T) Course In-charge: MOHAMMAD WASEEM AKRAM Course Seminar on “Norton’s Theorem” Presented by ✽ 28 CHAITALI UKE ✽ 29 CHAITALI INGALE
  • 2.
    Edward Lawry Norton Norton’sTheorem Statement: Any linear bilateral complicated circuit with multiple energy source and resistance can be replaced by a constant current source in parallel with a resistor connected across the load. IN ➳ The short-circuit current through the terminals RN ➳ Input/Equivalent resistance at the terminals when the independent source are turned off ➺ Norton's equivalent circuit
  • 3.
    Steps to SolveNorton’s Theorem 01 02 04 05 03 Identify the load resistance RL and short the load terminal of the circuit. By utilizing any network simplification technique, determine the current flowing through the shorted branch. This current will be the Norton’s current, IN. Now remove RL from the give circuit and replace all the active sources with their equivalent internal resistance. Further, evaluate the equivalent resistance across the open ends of the circuit. This resistance will be the Norton’s equivalent resistance RN. Now, draw Norton's equivalent circuit, comprising of IN in parallel combination with RN across the load resistance RL. Then find the current through the load resistance RL using:
  • 4.
    Consider the circuitshowm below: Numerical Implementation of Norton’s Theorem ➠ IN ↻ i1 i2 i3 For mesh 1, 50 = 5 i1 + 5 (i1 - i2 ) 50 = 10 i1 - 5 i2 For mesh 2, 0 = 10 i2 + 5 (i2 – i1 ) + 5 (i2 – i3 ) 0 = 5i1 - 20 i2 - 5 i3 For mesh 3, 0 = 5 (i3 – i2 ) i2 = i3 = N = 2A
  • 5.
    For calculating RN: NumericalImplementation of Norton’s Theorem ➠ RN RN = {( 5 II 5 ) + 10} II 5 RN = {( 5∗5 5+5 ) + 10} II 5 RN = {( 2.5) + 10} II 5 RN = ( 12.5) II 5 RN = ( 12.5∗5 12.5+5 ) RN = 3.5 Ω
  • 6.
    Numerical Implementation ofNorton’s Theorem Norton's Equivalent Circuit: IL = NRN RN+RL = 2 ∗ 3.5 2 + 3.5 = 1.27A
  • 7.