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Chapter 10 Sinusoidal Steady-State Analysis

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Presentation on theme: "Chapter 10 Sinusoidal Steady-State Analysis"— Presentation transcript:

1 Chapter 10 Sinusoidal Steady-State Analysis

2 Charles P. Steinmetz (1865-1923), the developer of the
mathematical analytical tools for studying ac circuits. Courtesy of General Electric Co.

3 Heinrich R. Hertz ( ). Courtesy of the Institution of Electrical Engineers. cycles/second Hertz, Hz

4 Sinusoidal voltage source vs  Vm sin(t  ).
Sinusoidal Sources Amplitude Period = 1/f Phase angle Angular or radian frequency = 2pf = 2p/T Sinusoidal voltage source vs  Vm sin(t  ). Sinusoidal current source is  Im sin(t  ).

5 Voltage and current of a circuit element.
Example v i circuit element + v _ i Voltage and current of a circuit element. The current leads the voltage by  radians OR The voltage lags the current by  radians

6 Example Find their phase relationship and Therefore the current leads the voltage by

7 Recall Triangle for A and B of Eq , where C 

8 Example A B B A

9 An RL circuit. Steady-State Response of an RL circuit
From #8&#9 Substitute the assumed solution into Coeff. of cos Coeff. of sin Solve for A & B

10 Steady-State Response of an RL circuit (cont.)
Thus the forced (steady-state) response is of the form

11 Complex Exponential Forcing Function
Input Response magnitude phase frequency Exponential Signal Note

12 Complex Exponential Forcing Function (cont.)
try We get where

13 Complex Exponential Forcing Function (cont.)
Substituting for A We expect

14 Example We replace Substituting ie

15 Example(cont.) The desired answer for the steady-state current interchangeable Or

16 Using Complex Exponential Excitation to Determine a
Circuit’s SS Response to a Sinusoidal Source Write the excitation as a cosine waveform with a phase angle Introduce complex excitation Use the assumed response Determine the constant A

17 Obtain the solution The desired response is Example

18 Example (cont.)

19 Example (cont.) The solution is The actual response is

20 The Phasor Concept A sinusoidal current or voltage at a given frequency is characterized by its amplitude and phase angle. Magnitude Phase angle Thus we may write unchanged

21 The Phasor Concept(cont.)
A phasor is a complex number that represents the magnitude and phase of a sinusoid. phasor The Phasor Concept may be used when the circuit is linear , in steady state, and all independent sources are sinusoidal and have the same frequency. A real sinusoidal current phasor notation

22 The Transformation Time domain Transformation Frequency domain

23 The Transformation (cont.)
Time domain Transformation Frequency domain

24 Example Substitute into Suppress

25 Example (cont.)

26 Phasor Relationship for R, L, and C Elements
Time domain Resistor Frequency domain Voltage and current are in phase

27 Inductor Time domain Frequency domain Voltage leads current by

28 Capacitor Time domain Frequency domain Voltage lags current by

29 Impedance and Admittance
Impedance is defined as the ratio of the phasor voltage to the phasor current. Ohm’s law in phasor notation phase magnitude or polar exponential rectangular

30 Graphical representation of impedance
Resistor wL Inductor Capacitor 1/wC

31 Admittance is defined as the reciprocal of impedance.
conductance In rectangular form susceptance G Resistor 1/wL Inductor wC Capacitor

32 Kirchhoff’s Law using Phasors
KVL KCL Both Kirchhoff’s Laws hold in the frequency domain. and so all the techniques developed for resistive circuits hold Superposition Thevenin &Norton Equivalent Circuits Source Transformation Node & Mesh Analysis etc.

33 Impedances in series Admittances in parallel

34 Example 10.9-1 R = 9 W, L = 10 mH, C = 1 mF i = ?
KVL

35 Example v = ? KCL

36 Node Voltage & Mesh Current using Phasors
va = ? vb = ?

37 KCL at node a KCL at node b Rearranging Admittance matrix

38 If Im = 10 A and Using Cramer’s rule to solve for Va Therefore the steady state voltage va is

39 Example v = ? use supernode concept as in #4

40 Example (cont.) KCL at supernode Rearranging

41 Example (cont.) Therefore the steady state voltage v is

42 Example i1 = ?

43 Example (cont.) KVL at mesh 1 & 2 Using Cramer’s rule to solve for I1

44 Superposition, Thevenin & Norton Equivalents
and Source Transformations Example i = ? Consider the response to the voltage source acting alone = i1

45 Example (cont.) Substitute

46 Example (cont.) Consider the response to the current source acting alone = i2 Using the principle of superposition

47 Source Transformations

48 Example IS = ?

49 Example 10.11-3 Thevenin’s equivalent circuit
?

50 Example 10.11-4 Thevenin’s equivalent circuit

51 Example 10.11-4 Norton’s equivalent circuit
?

52 Phasor Diagrams A Phasor Diagram is a graphical representation of phasors and their relationship on the complex plane. Take I as a reference phasor The voltage phasors are

53 Phasor Diagrams (cont.)
KVL For a given L and C there will be a frequency w that Resonant frequency Resonance

54 Summary Sinusoidal Sources
Steady-State Response of an RL Circuit for Sinusoidal Forcing Function Complex Exponential Forcing Function The Phasor Concept Impedance and Admittance Electrical Circuit Laws using Phasors


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