1 Lecture #4 EGR 272 – Circuit Theory II Read: Chapter 9 and Appendix B in Electric Circuits, 6 th Edition by Nilsson Sinusoidal Steady-State Analysis.

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Presentation transcript:

1 Lecture #4 EGR 272 – Circuit Theory II Read: Chapter 9 and Appendix B in Electric Circuits, 6 th Edition by Nilsson Sinusoidal Steady-State Analysis also called AC Circuit Analysis also called Phasor Analysis Discuss each name. Before beginning a study of AC circuit analysis, it is helpful to introduce (or review) two related topics: 1)sinusoidal waveforms 2)complex numbers

2 Lecture #4 EGR 272 – Circuit Theory II Sinusoidal Waveforms In general, a sinusoidal voltage waveform can be expressed as: v(t) = V p cos(wt) where V p = peak or maximum voltage w = radian frequency (in rad/s) T = period (in seconds) f = frequency in Hertz (Hz) Example: An AC wall outlet has V RMS = 120V and f = 60 Hz. Express the voltage as a time function and sketch the voltage waveform.

3 Lecture #4 EGR 272 – Circuit Theory II Shifted waveforms: v(t) = V p cos(wt +  )  = phase angle in degrees a shift to the left is positive and a shift to the right is negative (as with any function ) Example: Sketch v(t) = 50cos(500t – 30 o ) Radians versus degrees: Note that the argument of the cosine in v(t) = V p cos(wt +  ) has mixed units – both radians and degrees. If this function is evaluated at a particular time t, care must be taken such that the units agree. Example: Evaluate v(t) = 50cos(500t – 40 o ) at t = 1ms.

4 Lecture #4 EGR 272 – Circuit Theory II Relative shift between waveforms: V 1 leads V 2 by  or V 2 lags V 1 by  Example: v 1 (t) = 50cos(500t – 50 o ) and v 2 (t) = 40cos(500t + 60 o ). A)Does v 1 lead or lag v 2 ? By how much? B)If v 1 was shifted 0.5ms to the right, find a new expression for v 1 (t). C)If v 1 was shifted 0.5ms to the left, find a new expression for v 1 (t). D)By how many ms should v 1 be shifted to the right such that v 1 (t) = 50sin(500t)?

5 Lecture #4 EGR 272 – Circuit Theory II Complex Numbers A complex number can be expressed in two forms: 1)Rectangular form 2)Polar form A complex number X can be plotted on the complex plane, where x-axis: real part of the complex number y-axis: imaginary (j) part of the complex number

6 Lecture #4 EGR 272 – Circuit Theory II Rectangular Numbers A rectangular number specifies the x,y location of complex number X in the complex plane in the form: Example: X = 20 + j10

7 Lecture #4 EGR 272 – Circuit Theory II Polar Numbers A polar number specifies the distance and angle of complex number X from the origin in the complex plane in the form: Example: X = 20  30 o

8 Lecture #4 EGR 272 – Circuit Theory II Converting between rectangular form and polar form: Polar to Rectangular:Rectangular to Polar: Given: |X|,  Given: A, B Find: A, BFind: |X|,  Example: Convert X = 20  30 o to rectangular form. A = |X|cos(  ) B = |X|sin(  ) Example: Convert X = 20 + j10 to polar form. Complex numbers using calculators Refer to the handout entitled “Complex Numbers”

9 Lecture #4 EGR 272 – Circuit Theory II Mathematical Operations Using Complex Numbers Note: Calculators are used for most numerical calculations. When symbolic calculations are used, the following items may be helpful. 1) Addition/Subtraction – easiest in rectangular form

10 Lecture #4 EGR 272 – Circuit Theory II 2) Multiplication/Division – easiest in polar form 3) Inversion

11 Lecture #4 EGR 272 – Circuit Theory II 4) Exponentiation 5) Conjugate Example:

12 Lecture #4 EGR 272 – Circuit Theory II Example: Convert to the other form or simplify. 1) -32) -j3 3)j64)-4/j 5)1/(j2)6)j 2 7)j 3 8)j 4 9)300 – j25010)250  -75° 11)(-3-j6) * 12)(250  -75°) * 13)(4 + j7) 2 14)(-4 + j6) -1