A sinusoidal current source (independent or dependent) produces a current

1. A sinusoidal current source (independent or dependent) produces a current That varies sinusoidally with time

3. We define the Root Mean Square value of v(t) or rms as

4. The Root Mean Square value of Expand using trigonometric identity

8. 9.2 The Sinusoidal Response Solution for i(t) should be a sinusoidal of frequency 3 We notice that only the amplitude andphasechange In this chapter, we develop a technique for calculating the response directly without solving the differential equation

9. Time Domain Complex Domain Deferential Equation Algebraic Equation

10. 9.3The phasor The phasor is a complex number that carries the amplitude and phase angle information of a sinusoidal function The phasor concept is rooted in Euler’s identity Euler’s identity relates the complex exponential function to the trigonometric function We can think of the cosine function as the real part of the complex exponential and the sine function as the imaginary part Because we are going to use the cosine function on analyzing the sinusoidal steady-state we can apply

11. We can move the coefficient Vm inside is a complex number define to be the phasor that carries the amplitude and phase angle of a given sinusoidal function The quantity Phasor Transform Were the notation Is read “ the phasor transform of

12. Summation Property of Phasor (can be shown)

14. Since Next we derive y using phsor method

16. The V-I Relationship for a Resistor Let the current through the resistor be a sinusoidal given as Is also sinusoidal with amplitude And phase The sinusoidal voltage and current in a resistor are in phase

17. Phasor Transform Phasor Transform Now let us see the pharos domain representation or pharos transform of the current and voltage Which is Ohm’s law on the phasor ( or complex ) domain

18. The voltage and the current are in phase Imaginary Real

19. The V-I Relationship for an Inductor Let the current through the resistor be a sinusoidal given as The sinusoidal voltage and current in an inductor are out of phase by 90o The voltage lead the current by 90oor the current lagging the voltage by 90o You can express the voltage leading the current by T/4 or1/4fseconds wereTis the period and fis the frequency

20. Now we rewrite the sin function as a cosine function ( remember the phasor is defined in terms of a cosine function) The pharos representation or transform of the current and voltage But since Therefore and

21. and The voltage lead the current by 90oor the current lagging the voltage by 90o Imaginary Real

22. The V-I Relationship for a Capacitor Let the voltage across the capacitor be a sinusoidal given as The sinusoidal voltage and current in an inductor are out of phase by 90o The voltage lag the current by 90oor the current leading the voltage by 90o

23. The V-I Relationship for a Capacitor The pharos representation or transform of the voltage andcurrent and

24. and The voltage lag the current by 90oor the current lead the voltage by 90o Imaginary Real

25. Phasor ( Complex or Frequency) Domain Time-Domain

26. Impedance and Reactance The relation between the voltage and current on the phasor domain (complex or frequency) for the three elements R, L, and C we have When we compare the relation between the voltage and current , we note that they are all of form: Which the state that the phasor voltage is some complex constant ( Z ) times the phasor current This resemble ( شبه) Ohm’s law were the complex constant ( Z ) is called “Impedance” (أعاقه ) Recall on Ohm’s law previously defined , the proportionality content R was real and called “Resistant” (مقاومه ) Solving for ( Z ) we have The Impedance of a resistor is In all cases the impedance is measured in Ohm’s W The Impedance of an indictor is The Impedance of a capacitor is

27. Impedance The Impedance of a resistor is In all cases the impedance is measured in Ohm’s W The Impedance of an indictor is The Impedance of a capacitor is The imaginary part of the impedance is called “reactance” The reactance of a resistor is We note the “reactance” is associated with energy storage elements like the inductor and capacitor The reactance of an inductor is The reactance of a capacitor is Note that the impedance in general (exception is the resistor) is a function of frequency At w = 0 (DC), we have the following short open

28. Time Domain Phasor (Complex) Domain

31. 9.5 Kirchhoff’s Laws in the Frequency Domain ( Phasor or Complex Domain) Consider the following circuit PhasorTransformation KVL Using Euler Identity we have Which can be written as Factoring Can not be zero Phasor KVL on the phasor domain So in general

32. Kirchhoff’s Current Law A similar derivation applies to a set of sinusoidal current summing at a node Phasor Transformation KCL KCL on the phasor domain

33. 9.6 Series, Parallel, Simplifications and Ohm’s law in the phosor domain

34. Example 9.6 for the circuit shown below the source voltage is sinusoidal (a) Construct the frequency-domain (phasor, complex) equivalent circuit ? (b) Calculte the steady state current i(t) ? The source voltage pahsor transformation or equivalent The Impedance of the indictor is The Impedance of the capacitor is

35. To Calculate the phasor current I

36. and Ohm’s law in the phosor domain

37. Example 9.7 Combining Impedances in series and in Parallel (a) Construct the frequency-domain (phasor, complex) equivalent circuit ? (b) Find the steady state expressions for v,i1, i2, and i3 ? ? (a)

39. Delta-to Wye Transformations D to Y Y toD

40. Example 9.8

42. 9.7 Source Transformations and Thevenin-Norton Equivalent Circuits Source Transformations Thevenin-Norton Equivalent Circuits

43. Example 9.9

46. Example 9.10 Source Transformation KVL Since then Next we find the Thevenin Impedance

47. Thevenin Impedance

48. 9.8 The Node-Voltage Method Example 9.11 KCL at node 1 (1) KCL at node 2 Since (2) Two Equations and Two Unknown , solving

49. To Check the work

50. 9.9 The Mesh-Current Method Example 9.12 KVL at mesh 1 (1) KVL at mesh 2 Since (2) Two Equations and Two Unknown , solving