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Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 2
Session 12C: Focus
 Thévenin’s Theorem
◦ Example Problem 2
 Norton’s Theorem
 Home Work problem
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 3
Example 2: Thévenin’s Theorem
 Find current through 2 Ω:
4 Ω
6 Ω
4 Ω
5 Ω
9 V
4
9
4+ 4 + 6
2.571 V
6 Ω
4 Ω 4 Ω
5 Ω
2.571 V
7.857 Ω
2 Ω
voc = 2.571 V, RTH = 7.857 Ω I2Ω = 260.8 mA
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 4
A few Key Points: Thévenin Theorem
 The equivalent circuit that we have learnt to obtain, is
completely independent of network B
◦ To which the network A is connected to
 The only restriction that we must impose on A or B is that all
dependent sources in A have their control variables in A, and
similarly for B.
 No restrictions are imposed on the complexity of A or B;
either one may contain any combination of independent
voltage or current sources, linear dependent voltage or
current sources, resistors, or any other circuit elements which
are linear.
 The dead network A can be represented by a single
equivalent resistance RTH
◦ Which we will call the Thévenin equivalent resistance.
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com
Norton’s Equivalent Circuit
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 6
Example 3: Thévenin and Nortan’s equivalent
circuits
Find the Thévenin and Nortan’s equivalent circuits:
Applying Superposition to find Voc
= 5 kΩ
Voc
o
o
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 7
Example 3: Continued.
RTH = 5 kΩ
Voc = 8 V
Isc = 1.6 mA
Thévenin Equivalent circuit Norton Equivalent circuit
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 8
Norton’s Theorem
1. Given any linear circuit, rearrange it in the form of
two networks, A and B, connected by two wires.
◦ Network A is the network to be simplified; B will be left
untouched. As before, if either network contains a
dependent source, its controlling variable must be in the
same network.
2. Disconnect network B, and short the terminals of A.
Define a current isc as the current now flowing
through the shorted terminals of network A.
3. Turn off or “zero out” every independent source in
network A to form an inactive network (RTh).
Leave dependent sources unchanged.
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 9
Norton’s Theorem
4. Connect an independent current source with value isc
in parallel with the inactive network.
◦ Do not complete the circuit; leave the two terminals
disconnected.
5. Connect network B to the terminals of the new
network A.
◦ All currents and voltages in B will remain unchanged.
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com
Home Work Problem
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 11
HW1: Thévenin and Norton Equivalents
Note: This is Practice 5.7 on page 147, Figure 5.30 in the Ref 1 book (by Hayt)
voc = -7.86 V, RTH = 2.429 kΩ
Isc = -3.235 mA
Voc
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 12
Session 12C: Summary
 Thévenin’s and Norton’s Equivalent Circuit
 Thévenin’s Theorem
◦ Example Problem 2
 Norton’s Theorem
 Home Work problem
Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 13
References
Ref 1 Ref 2

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Basic Electric Circuits Session 12C

  • 1. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com
  • 2. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 2 Session 12C: Focus  Thévenin’s Theorem ◦ Example Problem 2  Norton’s Theorem  Home Work problem
  • 3. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 3 Example 2: Thévenin’s Theorem  Find current through 2 Ω: 4 Ω 6 Ω 4 Ω 5 Ω 9 V 4 9 4+ 4 + 6 2.571 V 6 Ω 4 Ω 4 Ω 5 Ω 2.571 V 7.857 Ω 2 Ω voc = 2.571 V, RTH = 7.857 Ω I2Ω = 260.8 mA
  • 4. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 4 A few Key Points: Thévenin Theorem  The equivalent circuit that we have learnt to obtain, is completely independent of network B ◦ To which the network A is connected to  The only restriction that we must impose on A or B is that all dependent sources in A have their control variables in A, and similarly for B.  No restrictions are imposed on the complexity of A or B; either one may contain any combination of independent voltage or current sources, linear dependent voltage or current sources, resistors, or any other circuit elements which are linear.  The dead network A can be represented by a single equivalent resistance RTH ◦ Which we will call the Thévenin equivalent resistance.
  • 5. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com Norton’s Equivalent Circuit
  • 6. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 6 Example 3: Thévenin and Nortan’s equivalent circuits Find the Thévenin and Nortan’s equivalent circuits: Applying Superposition to find Voc = 5 kΩ Voc o o
  • 7. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 7 Example 3: Continued. RTH = 5 kΩ Voc = 8 V Isc = 1.6 mA Thévenin Equivalent circuit Norton Equivalent circuit
  • 8. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 8 Norton’s Theorem 1. Given any linear circuit, rearrange it in the form of two networks, A and B, connected by two wires. ◦ Network A is the network to be simplified; B will be left untouched. As before, if either network contains a dependent source, its controlling variable must be in the same network. 2. Disconnect network B, and short the terminals of A. Define a current isc as the current now flowing through the shorted terminals of network A. 3. Turn off or “zero out” every independent source in network A to form an inactive network (RTh). Leave dependent sources unchanged.
  • 9. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 9 Norton’s Theorem 4. Connect an independent current source with value isc in parallel with the inactive network. ◦ Do not complete the circuit; leave the two terminals disconnected. 5. Connect network B to the terminals of the new network A. ◦ All currents and voltages in B will remain unchanged.
  • 10. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com Home Work Problem
  • 11. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 11 HW1: Thévenin and Norton Equivalents Note: This is Practice 5.7 on page 147, Figure 5.30 in the Ref 1 book (by Hayt) voc = -7.86 V, RTH = 2.429 kΩ Isc = -3.235 mA Voc
  • 12. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 12 Session 12C: Summary  Thévenin’s and Norton’s Equivalent Circuit  Thévenin’s Theorem ◦ Example Problem 2  Norton’s Theorem  Home Work problem
  • 13. Basic Electric Circuits – © 2020 Mouli Sankaran Email: mouli.sankaran@yahoo.com 13 References Ref 1 Ref 2