Sinusoids and Phasors Chapter 9 George Westinghoues (1946-1914) ch09_Sinusoids and Phasors 2 9.2 Sinusoids • Consider the sinusoidal voltage v(t) = Vm sint where Vm = the amplitude of the sinusoid = the angular frequency in radians/s t = the argument of the sinusoid T ch09_Sinusoids and Phasors 2 3 Fig 9.1 2 v(t T ) Vm sin (t T ) Vm sin t Vm sin(t 2 ) Vm sin t v(t ) Hence, v(t T ) v(t ) ch09_Sinusoids and Phasors 4 Fig 9.2 ch09_Sinusoids and Phasors 5 Example 9.1 • Find the amplitude, phase, period, and frequency of the sinusoid v(t) = 12cos(50t + 10°) • Solution: The amplitude is Vm = 12V. The phase is = 10° 2 2 0.1257 s. The period T 50 The frequency is f 1 7.958 Hz. T ch09_Sinusoids and Phasors 6 Example 9.2 • Calculus the phase angle between v1 = -10 cos (t + 50°) and v2 = 12 sin (t - 10°). State which sinusoid is leading. • Solution: v1 = -10 cos (t + 50°) = 10 cos (t + 50° - 180°) v1 = 10 cos (t - 130°) or v1 = 10 cos (t + 130°) and v2 = 12 sin (t - 10°) = 12 cos (t - 10° - 90°) v2 = 12cos (t - 100°) . The phase difference between v1 and v2 is 30°. We can write v2 as v2 = 12 cos (t - 130° + 30°) or v2 = 12 cos (t + 260°) ch09_Sinusoids and Phasors 7 9.3 Phasor • A phasor is a complex number that represents the amplitude and phase of a sinusoid. z x jy z r re j z x jy Rectangular form z r Polar form Exponential form z re j ch09_Sinusoids and Phasors 8 Fig 9.6 z x yj r r (cos j sin ) ch09_Sinusoids and Phasors 9 • Addition: z1 z2 ( x1 x2 ) j ( y1 y2 ) • Subtraction: z1 z2 ( x1 x2 ) j ( y1 y2 ) • Multiplication: • Division: ch09_Sinusoids and Phasors z1 z2 r1r2(1 2 ) z1 r1 (1 2 ) z2 r2 10 • Reciprocal: 1 1 ( ) z r • Square Root: z r( / 2) • Complex Conjugate: z x jy r( ) re * ch09_Sinusoids and Phasors j 11 e j cos j sin cos Re(e j ) sin Im( e j ) v(t ) Vm cos(t ) Re(Vme j (t ) ) v(t ) Re(Vme j e jt ) v(t ) Re(Ve jt ) where V Vme j Vm ch09_Sinusoids and Phasors 12 Fig 9.7 ch09_Sinusoids and Phasors 13 (Time-domain representation) Phasor-domain representation) v(t ) Vm cos(t ) V Vm ch09_Sinusoids and Phasors 14 Table 9.1 Sinusoid-phasor transformation Time domain representation Phasor domain representation Vm cos(t ) Vm Vmsin(t ) Vm( 90) I m cos(t ) I m I m sin(t ) I m( 90) ch09_Sinusoids and Phasors 15 Example 9.3 • Evaluate these complex numbers: 1/ 2 (a) (4050 20 30) 10 30 (3 j 4) (b) (2 j 4)(3 j 5) * • Solution: (a) 4050 40(cos 50 j sin 50) 25.71 j 30.64 20 30 20[cos( 30) j sin(30)] 17.32 j10 4050 20 30 43.03 j 20.64 47.7225.63 (4050 20 30)1/ 2 6.9112.81 ch09_Sinusoids and Phasors 16 Example 9.3 10 30 (3 j 4) 8.66 j 5 (3 4 j ) (b) (2 j 4)(3 j 5) * (2 j 4)(3 j 5) 11.33 j 9 14.73 37.66 14 j 22 26.08122.47 0.565 160.13 ch09_Sinusoids and Phasors 17 Example 9.4 • Transform these sinusoid to phasors: (a) i 6 cos(50t 40) A (b) v 4 sin(30t 50) V • Solution: (a) i 6 cos(50t 40) has the phasor I 6 40 A (b) Since sinA cos( A 90) v 4 sin(30t 50) 4 cos(30t 50 90) 4 cos(30t 140) V The Phasor form of v is V 4140 V ch09_Sinusoids and Phasors 18 Example 9.5 • Find the sinusoid representation by these phasors: (a) I 3 j 4 A (b) V j8e j 20 V • Solution: (a) I 3 j 4 5126.87 i (t ) 5 cos(t 126.87) A (b) j 190, V j8 20 (190)(8 20) 890 20 870 V v(t ) 8 cos(t 70) V ch09_Sinusoids and Phasors 19 9.4 Phasor Relationships for Circuit Elements v iR RI m cos(t ) V RI m V RI ch09_Sinusoids and Phasors 20 Fig 9.9 ch09_Sinusoids and Phasors 21 Fig 9.10 ch09_Sinusoids and Phasors 22 di v L LI m sin(t ) dt sin A cos( A 90), v LI m cos(t 90) V LI me j ( 90) LI me j e j 90 LI m( 90) But I m I, e j 90 j , then V jLI. ch09_Sinusoids and Phasors 23 Fig 9.11 ch09_Sinusoids and Phasors 24 Fig 9.12 ch09_Sinusoids and Phasors 25 dv iC dt I jCV V ch09_Sinusoids and Phasors I jC 26 Fig 9.13 ch09_Sinusoids and Phasors 27 Fig 9.14 ch09_Sinusoids and Phasors 28 Table 9.2 Summary of voltagecurrent relationships Element Time domain Frequency domain R V = Ri V =RI L di vL dt V = jLI C dv iC dt ch09_Sinusoids and Phasors V I jC 29 Example 9.8 • The voltage c = 12 cos(60t + 45°) is applied to a 0.1H inductor. Find the steady-state current through the inductor. • Solution: V jLI, where 60rad/s and V 1245 V. Hence, V 1245 1245 I 2 45 A jL j 60 0.1 690 Converting , i (t ) 2 cos(60t 45) A ch09_Sinusoids and Phasors 30 9.5 Impedance and Admittance V Z I or V ZI • The impedance Z of a circuit is the ratio of the phasor voltage V to the phasor current I, measured in ohms (Ω). ch09_Sinusoids and Phasors 31 Table 9.3 Impedance and admittances of passive elements Element R L C ch09_Sinusoids and Phasors Impedance Admittances Z=R 1 Y R Z = jL Z I jC Y I jL Y = jC 32 Fig 9.15 ch09_Sinusoids and Phasors 33 Z R jX Z where X Z R X , tan R 2 2 1 and R Z cos , ch09_Sinusoids and Phasors X Z sin 34 Example 9.9 • Find v(t) and i(t) in the circuit shown in Fig. 9.16. ch09_Sinusoids and Phasors 35 Example 9.9 • From the voltage source 10 cos 4t, = 4, Vs 100 V • The impedance is 1 1 Z 5 5 5 j 2.5 jC j 4 0.1 • Hence the current Vs 100 10(5 j 2.5) I 2 Z 5 j 2.5 5 2.52 1.6 j 0.8 1.78926.57 A ch09_Sinusoids and Phasors 36 Example 9.9 • The voltage across the capacitor is 1.78926.57 V IZ C jC j 4 0.1 1.78926.57 4.47 63.43 V 0.490 • Converting I and V, we get I i (t ) 1.789 cos(4t 26.57) A v() 4.47 cos(4t 63.43) V ch09_Sinusoids and Phasors 37 9.6 Kirchhoff’s Law in the Frequency Domain V1 V2 Vn 0 I1 I 2 I n 0 ch09_Sinusoids and Phasors 38 9.7 Impedance Combinations V V1 V2 VN I (Z1 Z 2 Z N ) V Z eq Z1 Z 2 Z N I ch09_Sinusoids and Phasors 39 Fig 9.19 V I Z1 Z 2 Since V1 Z1I and V2 Z 2I, then Z1 Z2 V1 V, V2 V Z1 Z 2 Z1 Z 2 ch09_Sinusoids and Phasors 40 Fig 9.20 1 1 1 I I1 I 2 I N V ZN Z1 Z 2 1 I 1 1 1 Z eq V Z1 Z 2 ZN Yeq Y1 Y2 YN ch09_Sinusoids and Phasors 41 Fig 9.21 1 1 1 Z1Z 2 Z eq Yeq Y1 Y2 1/Z1 1 / Z 2 Z1 Z 2 V IZ eq I1Z1 I 2 Z 2 Z2 Z1 I1 I, I 2 I Z1 Z 2 Z1 Z 2 ch09_Sinusoids and Phasors 42 Fig 9.22 ch09_Sinusoids and Phasors 43 • Y-Δ Conversion Z1Z 2 Z 2 Z3 Z3Z1 Za Z1 Z1Z 2 Z 2 Z3 Z3Z1 Zb Z2 Z1Z 2 Z 2 Z3 Z3Z1 Zc Z3 ch09_Sinusoids and Phasors 44 • Δ-Y Conversion Ζb Z c Z1 Z a Zb Z c Ζc Za Z2 Z a Zb Z c Ζ a Zb Z3 Z a Zb Z c ch09_Sinusoids and Phasors 45 Example 9.10 • Find the input impedance of the circuit in Fig. 9.23. Assume that the circuit operations at = 50 red/s. ch09_Sinusoids and Phasors 46 Example 9.10 Let Z1 = Impedance of the 2-mF capacitor. Z2 = Impedance of the 3-Ω resistor in series with the 10-mF capacitor Z3 = Impedance of the 0.2-H inductor in series with the 8-Ω resisotr 1 1 Z j10 Then 1 3 jC j 50 2 10 1 1 Z2 3 3 (3 j 2) 3 jC j 50 10 10 1 Z3 8 8 j 50 0.2 (8 j10) jC ch09_Sinusoids and Phasors 47 Example 9.10 The input impedance is (3 j 2)(8 j10) Zin Z1 Z 2 Z3 j10 11 j8 (44 j14)(11 j8) j10 j10 3.22 j1.07 2 2 11 8 Thus Zin 3.22 j11.07 ch09_Sinusoids and Phasors 48 Example 9.11 • Determine v0(t) in the circuit of Fig. 9.25. ch09_Sinusoids and Phasors 49 Example 9.11 vs 20 cos( 4t 15) Vs 20 15 V, 4 1 1 10mF jC j 4 10 103 5 H jL j 4 5 j 20 ch09_Sinusoids and Phasors 50 Example 9.11 Let Z1 = Impedance of the 60-Ω resistor Z2 = Impedance of the parallel combination of the 10mF capacitor and the 5-H inductor Then Z1 = 60 Ω and j 25 j 20 Z 2 j 25 j 20 j100 j 25 j 20 ch09_Sinusoids and Phasors 51 Example 9.11 By the voltage-division principle, Z2 j100 Vo Vz (20 15) Z1 Z 2 60 j100 (0.857530.96)( 20 15) 17.1515.96 V We converting this to the time domain and obtain vo (t ) 17.15 cos(4t 15.96) V ch09_Sinusoids and Phasors 52