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Useful Circuit Analysis Techniques

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1 Useful Circuit Analysis Techniques
Chapter 5: Useful Circuit Analysis Techniques 1 Dr. Amer Alsaraira

2 Objectives : Superposition Source transformation
the Thevenin equivalent of any network the Norton equivalent of any network the load resistance that will result in maximum power transfer 2 Dr. Amer Alsaraira

3 Linearity and Superposition :
Linear Elements and Linear Circuits a linear element is a passive element that has a linear voltage-current relationship. a linear dependent source is a dependent current or voltage source whose output current or voltage is proportional only to the first power of a specified current or voltage variable in the circuit (or to the sum of such quantities). a linear circuit is a circuit composed entirely of independent sources, linear dependent sources, and linear elements. 3 Dr. Amer Alsaraira

4 The principle of superposition :
The response in a linear circuit having more than one independent source can be obtained by adding the responses caused by the separate independent sources acting alone. (a) A voltage source set to zero acts like a short circuit. (b) A current source set to zero acts like an open circuit. 4 Dr. Amer Alsaraira

5 Example 5.1: Use superposition to find the current ix. 5
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6 Practice: 5.1 Use superposition to find the current Ix. 6
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7 Example 5.3 : Use superposition to find the current Ix. 7
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8 Example 5.3 : Use superposition to find the current Ix. 8
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9 Practice: 5.2 Use superposition to obtain the voltage
across each current source. 9 Dr. Amer Alsaraira

10 Source Transformation:
(a) A general practical voltage source connected to a load resistor RL. (b) The terminal characteristics compared to an ideal source. (a) A general practical current source connected to a load resistor RL. (b) The terminal characteristics compared to an ideal source. 10 Dr. Amer Alsaraira

11 Equivalent Sources: 11 Dr. Amer Alsaraira

12 Equivalent Sources: 12 Dr. Amer Alsaraira

13 Example 5.4: Compute the current through the 4.7 k resistor after transforming the 9 mA source into an equivalent voltage source. 13 Dr. Amer Alsaraira

14 Practice: 5.3 compute the current ix after performing a source
transformation on the voltage source 14 Dr. Amer Alsaraira

15 Example 5.5: Calculate the current through the 2Ω resistor 15
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16 Practice: 5.4 Compute the voltage V 16 Dr. Amer Alsaraira

17 Thevenin and Norton Equivalent:
A complex network including a load resistor RL. A Thévenin equivalent network connected to RL. A Norton equivalent network connected to RL. 17 Dr. Amer Alsaraira

18 Thevenin’s theorem: Given any linear circuit, rearrange it in the form
of two networks A and B connected by two wires. Define a voltage voc as the open-circuit voltage which appears across the terminals of A when B is disconnected. Then all currents and voltages in B will remain unchanged if all independent voltage and current sources in A are “killed” or “zeroed out,” and an independent voltage source voc is connected, with proper polarity, in series with the dead (inactive) A network. 18 Dr. Amer Alsaraira

19 Example 5.6: Determine the Thevenin equivalent. 19 Dr. Amer Alsaraira

20 Example 5.7: Determine the Thevenin equivalent. (use Theory) 20
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21 Practice: 5.5 Using repeated source transformations,
determine the Thevenin equivalent of the highlighted network 21 Dr. Amer Alsaraira

22 Practice: 5.6 Use Thevenin’s theorem to find the current
through the 2-c resistor 22 Dr. Amer Alsaraira

23 Example 5.8: Determine the Thevenin equivalent for the network faced by 1-kohm . 23 Dr. Amer Alsaraira

24 “killed” or “zeroed out,” and an independent current
Norton’s theorem: Given any linear circuit, rearrange it in the form of two networks A and B connected by two wires. If either network contains a dependent source, its control variable must be in that same network. Define a current isc as the short circuit current that appears when B is disconnected and the terminals of A are short-circuited. Then all currents and voltages in B will remain unchanged if all independent voltage and current sources in A are “killed” or “zeroed out,” and an independent current source isc is connected, with proper polarity, in parallel with the dead (inactive) A network 24 Dr. Amer Alsaraira

25 Example: Determine the Norton equivalent for the network
faced by 1-kohm . 25 Dr. Amer Alsaraira

26 Thevenin and Norton equivalents
26 Dr. Amer Alsaraira

27 Determine the Thevenin and Norton equivalents
Practice: 5.7 Determine the Thevenin and Norton equivalents 27 Dr. Amer Alsaraira

28 Example 5.9: Determine the Thevenin equivalent. 28 Dr. Amer Alsaraira

29 Example 5.9: Determine the Thevenin equivalent. 29 Dr. Amer Alsaraira

30 Practice: 5.8 Determine the Thevenin equivalent 30 Dr. Amer Alsaraira

31 Example 5.10: Find the Thévenin equivalent of the circuit shown. 31
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32 Practice: 5.9 Page 52 Determine the Thevenin equivalent 32
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33 Example 5.9: Determine the Thevenin equivalent resistance (RTH). 33
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34 Maximum Power Transfer:
34 Dr. Amer Alsaraira

35 Maximum Power Transfer:
35 Dr. Amer Alsaraira

36 Example: Select R1 so that maximum power is transferred from stage 1 to stage 2 and find the maximum power 36 Dr. Amer Alsaraira

37 Example 5.11: The circuit shown is a model for a common-emitter bipolar junction transistor amplifier. Choose a load resistance so that maximum power is transferred to it from the amplifier, and calculate the actual power absorbed. 37 Dr. Amer Alsaraira

38 Practice: 5.10 If Rout = 3kΩ, find the power delivered to it
What is the maximum power that can be delivered to any Rout 38 Dr. Amer Alsaraira


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