Chapter 6: Series-Parallel Circuits

Transcription

1 Chapter 6: Series-Parallel Circuits Instructor: Jean-François MILLITHALER Slide 1

2 Identifying series-parallel relationships Most practical circuits have combinations of series and parallel components. Components that are connected in series will share a common path. Components that are connected in parallel will be connected across the same two nodes. Slide 2

3 Combination circuits Most practical circuits have various combinations of series and parallel components. You can frequently simplify analysis by combining series and parallel components. An important analysis method is to form an equivalent circuit. An equivalent circuit is one that has characteristics that are electrically the same as another circuit but is generally simpler. Slide 3

4 Identifying series-parallel relationships Slide 4

5 Identifying series-parallel relationships Slide 5

6 Identifying series-parallel relationships Slide 6

7 Identifying series-parallel relationships Slide 7

8 Examples R T = R 1 + R 5 + R 4 (R 2 + R 3 ) R T = R 1 + R 2 R 3 + R 4 R 5 Slide 8

9 Total resistance Identifying the components Total resistance R T = R 1 + R 2 R 3 = = 60 W Slide 9

10 Example Find R T = 148 W Slide 10

11 Total Current 5 V Ohm s law: I T = V S R T Find I 4 = 3.45 ma (I 2 = 9.29 ma) Slide 11

12 Voltage Relationships Find R AB, R BC & R T Find V 1, V 2, V 3, V 4, and V 5 V 1 = V 2 = 5.15 V V 3 = 4.85 V V 4 = 1.58 V V 5 = 3.27 V Slide 12

13 Slide 13

14 THE WHEATSTONE BRIDGE Sir Charles Wheatstone, Used to precisely measure resistance Used also in conjunction with transducers Transducer = sensor. Change physical parameter in resistance, for example. Slide 14

15 THE WHEATSTONE BRIDGE The balanced bridge Balanced bridge when the output V OUT = 0V We have then V 1 =V 2 and V 3 =V 4 Therefore V 1 V 3 = V 2 V 4 and I 1 R 1 I 3 R 3 = I 2 R 2 I 4 R 4 Since I 1 = I 3 and I 2 = I 4 We got R 1 R 3 = R 2 R 4 and finally R 1 = R 3 R 2 R 4 Bridge to find an unknown resistance Slide 15

16 THE WHEATSTONE BRIDGE Example Determine the value of R X. The bridge is balanced (V OUT = 0 V) when R V is set at 1200 W R X = R V R 2 R 4 = = 1800 Ω Slide 16

17 THE WHEATSTONE BRIDGE The unbalanced bridge Unbalanced bridge when the output V OUT 0V Used to measure several types of physical quantities such as mechanical strain, temperature, or pressure. Connecting the transducer in one leg of the bridge. The resistance of the transducer changes proportionally to the changes in the parameter that it is measuring. If the bridge is balanced at a known point, then the amount of deviation indicates the amount of change in the parameter being measured. Therefore, the value of the parameter being measured can be determined by the amount that the bridge is unbalanced Slide 17

18 THE WHEATSTONE BRIDGE Example Determine the output voltage of the temperature-measuring bridge circuit if the thermistor is exposed to a temperature of 50ºC and its resistance at 25ºC is 1.0 kω. Assume the resistance of the thermistor decreases to 900 Ω at 50 C. At 25ºC the bridge is balanced. At 50ºC the bridge is unbalanced. We can apply the voltage-divider formula to the left and right sides. V A = R 3 R 3 +R therm V S = 1kΩ 1kΩ+900Ω 12 V = 6.32 V V B = R 4 V R 2 +R S = 1kΩ 4 2kΩ 12 V = 6. V V OUT = V A -V B = = 0.32 V at 50ºC Slide 18

19 Slide 19

20 THEVENIN s Theorem Léon Charles Thévenin, French Engineer, What for? To simplify Electric Engineer s Life!!! Simplify a complicate series-parallel circuit into an equivalent circuit Consists of an equivalent voltage source V TH And an equivalent resistance R TH Slide 20

21 THEVENIN s Theorem The Thevenin equivalent voltage V TH is the open circuit (no-load) voltage between two specified output terminals in a circuit. The Thevenin equivalent resistance R TH is the total resistance appearing between two specified output terminals in a circuit with all sources replaced by their internal resistances (which for an ideal voltage source is zero). Slide 21

22 Three steps: #1 Circuit complicate Output terminals Step 1: Find V TH = Find the voltage between A and B Slide 22

23 Three steps: #2 Step 2: Find R TH Short-circuiting the battery Find the resistance between A and B Slide 23

24 Three steps: #3 Step 3: Combining both V TH and R TH Thevenin equivalent circuit Slide 24

25 Depends on the viewpoint Slide 25

26 Depends on the viewpoint Slide 26

27 Thevenizing a Bridge Circuit Slide 27

28 Slide 31

29 Maximum Power Transfer Theorem For a given source voltage, maximum power is transferred from a source to a load when the load resistance is equal to the internal source resistance. Maximum power is transferred to the load when R L = R S. Slide 32

30 Maximum Power Transfer Theorem Example: Determine the load power for different values of the variable load resistance [0:125] W Solution: Using Ohm s law and Power Formula For R L = 0 W I = V S = 10 = 133 ma R S + R L P L = I 2 R L = = 0 W Slide 33

31 Maximum Power Transfer Theorem P L (mw) 400 Maximum for R L =R S For R L = 0 W : P L = 0 W For R L = 25 W : P L = 250 mw 100 For R L = 50 W : P L = 320 mw For R L = 75 W : P L = 334 mw For R L = 100 W : P L = 326 mw R L (W) For R L = 125 W : P L = 313 mw Note that R S = R TH if we are using the Thevenin s Theorem Slide 34

32 Superposition Theorem What is happening when there are two or more voltage sources??? How do we calculate I 2??? Slide 35

33 Superposition Theorem Problem: Find I 2 Determine R T1 and I T1 Then I 2(S1) Determine R T2 and I T2 Then I 2(S2) I 2 = I 2(S1) + I 2(S2) Slide 36

34 Superposition Theorem Example Find I 2, the current through R 2 1_ short replace V S2, find R T1, then I T1 and finally I 2(S1) R T1 =232 W // I T1 = 43.1 ma // I 2(S1) =25.9 ma 2_ short replace V S1, find R T2, then I T2 and finally I 2(S2) R T1 =399 W // I T1 = 12.5 ma // I 2(S1) =3.9 ma I 2 = I 1(S1) + I 2(S2) = = 29.8 ma Slide 37