1. Fig 33-CO These large transformers are used to increase the voltage at a power plant for distribution of energy by electrical transmission to the power grid. Voltages can be changed relatively easily because power is distributed by alternating current rather than direct current. (Lester Lefkowitz/Getty Images)
Fig 33-CO, p.1033

2. amplitude, the angular frequency is
.. the basic principle of the ac generator is a direct consequence of Faraday’s law of induction. When a conducting loop is rotated in a magnetic field at constant angular frequency ω , a sinusoidal voltage (emf) is induced in the loop. This instantaneous voltage Δv is
where ΔV max is the maximum output voltage of the ac generator, or the voltage
amplitude, the angular frequency is
Figure 33.1 The voltage supplied by an AC source is sinusoidal with a period T.
where f is the frequency of the generator (the voltage source) and T is the period.
Commercial electric power plants in the United States use a frequency of 60 Hz, which corresponds to an angular frequency of 377 rad/s.
The voltage supplied by an AC source is sinusoidal with a period T.
Fig 33-1, p.1034

3. To simplify our analysis of circuits containing two or more elements, we use graphical constructions called phasor diagrams.
In these constructions, alternating (sinusoidal) quantities, such as current and voltage, are represented by rotating vectors called phasors.
The length of the phasor represents the amplitude (maximum value) of the quantity, and the projection of the phasor onto the vertical axis represents the instantaneous value of the quantity.
As we shall see, a phasor diagram greatly simplifies matters when we must combine several sinusoidally varying currents or voltages that have different phases.

4. At any instant, the algebraic sum of the voltages around a closed loop in a circuit must be zero (Kirchhoff’s loop rule).
where ΔvR is the instantaneous voltage across the resistor. Therefore, the instantaneous current in the resistor is
the maximum current:
Active Figure 33.2 A circuit consisting of a resistor of resistance R connected to an AC source, designated by the symbol
Fig 33-2, p.1035

5. Active Figure 33.3 (a) Plots of the instantaneous current iR and instantaneous voltage vR across a resistor as functions of time. The current is in phase with the voltage, which means that the current is zero when the voltage is zero, maximum when the voltage is maximum, and minimum when the voltage is minimum. At time t = T, one cycle of the time-varying voltage and current has been completed. (b) Phasor diagram for the resistive circuit showing that the current is in phase with the voltage.
Fig 33-3, p.1035

6. Plots of the instantaneous current iR and instantaneous voltage vR across a resistor as functions of time.
The current is in phase with the voltage, which means that the current is zero when the voltage is zero, maximum when the voltage is maximum, and minimum when the voltage is minimum.
At time t = T, one cycle of the time-varying voltage and current has been completed.
Active Figure 33.3 (a) Plots of the instantaneous current iR and instantaneous voltage vR across a resistor as functions of time. The current is in phase with the voltage, which means that the current is zero when the voltage is zero, maximum when the voltage is maximum, and minimum when the voltage is minimum. At time t = T, one cycle of the time-varying voltage and current has been completed.
Fig 33-3a, p.1035

7. Phasor diagram for the resistive circuit showing that the current is in phase with the voltage.
What is of importance in an ac circuit is an average value of current, referred to as the rms current
Active Figure 33.3 (b) Phasor diagram for the resistive circuit showing that the current is in phase with the voltage.
Fig 33-3b, p.1035

8. (a) Graph of the current in a resistor as a function of time
Figure 33.5 (a) Graph of the current in a resistor as a function of time. (b) Graph of the current squared in a resistor as a function of time. Notice that the gray shaded regions under the curve and above the dashed line for I 2 max/2 have the same area as the gray shaded regions above the curve and below the dashed line for I 2 max/2. Thus, the average value of i 2 is I 2 max/2.
(b) Graph of the current squared in a resistor as a function of time.
Notice that the gray shaded regions under the curve and above the dashed line for I 2max/2 have the same area as the gray shaded regions above the curve and below the dashed line for I 2 max/2. Thus, the average value of i 2 is I 2max/2.
Fig 33-5, p.1037

9. The voltage output of a generator is given by Δv = (200 V)sin ωt
The voltage output of a generator is given by Δv = (200 V)sin ωt. Find the rms current in the circuit when this generator is connected to a 100 Ω- resistor.

10. is the self-induced instantaneous voltage across the inductor.
Active Figure 33.6 A circuit consisting of an inductor of inductance L connected to an AC source.
Fig 33-6, p.1038

11. the inductive reactance

12. Active Figure 33.7 (a) Plots of the instantaneous current iL and instantaneous voltage vL across an inductor as functions of time. The current lags behind the voltage by 90°.
Fig 33-7a, p.1039

13. Active Figure 33.7 (b) Phasor diagram for the inductive circuit, showing that the current lags behind the voltage by 90°.
Fig 33-7b, p.1039

14. In a purely inductive ac circuit, L = 25
In a purely inductive ac circuit, L = 25.0 mH and the rms voltage is 150 V. Calculate the inductive reactance and rms current in the circuit if the frequency is 60.0 Hz.

17. Active Figure 33.9 A circuit consisting of a capacitor of capacitance C connected to an AC source.
Fig 33-9, p.1041

18. Active Figure (a) Plots of the instantaneous current iC and instantaneous Voltage  vC across a capacitor as functions of time. The voltage lags behind the current by 90°. (b) Phasor diagram for the capacitive circuit, showing that the current leads the voltage by 90°.
Fig 33-10, p.1041

19. Active Figure (a) Plots of the instantaneous current iC and instantaneous Voltage  vC across a capacitor as functions of time. The voltage lags behind the current by 90°.
Fig 33-10a, p.1041

20. Active Figure (b) Phasor diagram for the capacitive circuit, showing that the current leads the voltage by 90°.
Fig 33-10b, p.1041

21. capacitive reactance:

23. Φ the phase angle between the current and the applied voltage
the current at all points in a series ac circuit has the same amplitude and phase
Active Figure (a) A series circuit consisting of a resistor, an inductor, and a capacitor connected to an AC source.
Fig 33-13a, p.1044

25. Active Figure 33.13 (b) Phase relationships for instantaneous voltages in the series RLC circuit.
Fig 33-13b, p.1044

26. Figure Phase relationships between the voltage and current phasors for (a) a resistor, (b) an inductor, and (c) a capacitor connected in series.
Fig 33-14, p.1044

27. Figure 33.14 Phase relationships between the voltage and current phasors for (a) a resistor
Fig 33-14a, p.1044

28. Figure 33.14 Phase relationships between the voltage and current phasors for (b) an inductor
Fig 33-14b, p.1044

29. Figure Phase relationships between the voltage and current phasors for (c) a capacitor connected in series.
Fig 33-14c, p.1044

30. Active Figure (a) Phasor diagram for the series RLC circuit shown in Figure 33.13a. The phasor  VR is in phase with the current phasor Imax, the phasor  VL leads Imax by 90°, and the phasor VC lags Imax by 90°. The total voltage  Vmax makes an Angle  with Imax. (b) Simplified version of the phasor diagram shown in part (a).
(a) Phasor diagram for the series RLC circuit The phasor  VR is in phase with the current phasor Imax, the phasor  VL leads Imax by 90°, and the phasor VC lags Imax by 90°. The total voltage  Vmax makes an Angle  with Imax. (b) Simplified version of the phasor diagram shown in part (a)
Fig 33-15, p.1045

31. Figure An impedance triangle for a series RLC circuit gives the relationship Z R2 + (XL - XC)2.
An impedance triangle for a series RLC circuit gives the relationship Z R2 + (XL - XC)2
Fig 33-16, p.1045

32. Table 33-1, p.1046

34. the phase angle

40. No power losses are associated with pure capacitors and pure inductors in
an ac circuit
When the current begins to increase in one direction in an ac circuit, charge begins to accumulate on the capacitor, and a voltage drop appears across it. When this voltage drop reaches its maximum value, the energy stored in the capacitor is
However, this energy storage is only momentary. The capacitor is charged and discharged twice during each cycle: Charge is delivered to the capacitor during two quarters of the cycle and is returned to the voltage source during the remaining two quarters. Therefore, the average power supplied by the source is zero. In other words, no power losses occur in a capacitor in an ac circuit.

41. For the RLC circuit , we can express the instantaneous power P
The average power
the quantity cos φ is called the power factor
the maximum voltage drop across the resistor is given by

42. In words, the average power delivered by the generator is converted to internal energy in the resistor, just as in the case of a dc circuit. No power loss occurs in an ideal inductor or capacitor.
When the load is purely resistive, then φ= 0, cos φ= 1, and

44. A series RLC circuit is said to be in resonance when the current has its maximum value. In general, the rms current can be written
Because the impedance depends on the frequency of the source, the current in the RLC circuit also depends on the frequency. The frequency ω0 at which XL-XC=0 is called the resonance frequency of the circuit. To find ω0 , we use the condition XL = XC ,from which we obtain , ω0 L =1/ ω0 C or

45. Active Figure (a) The rms current versus frequency for a series RLC circuit, for three values of R. The current reaches its maximum value at the resonance frequency 0. (b) Average power delivered to the circuit versus frequency for the series RLC circuit, for two values of R.
(a) The rms current versus frequency for a series RLC circuit, for three values of R. The current reaches its maximum value at the resonance frequency 0. (b) Average power delivered to the circuit versus frequency for the series RLC circuit, for two values of R.
Fig 33-19, p.1050

46. Active Figure (a) The rms current versus frequency for a series RLC circuit, for three values of R. The current reaches its maximum value at the resonance frequency 0.
Fig 33-19a, p.1050

47. Active Figure (b) Average power delivered to the circuit versus frequency for the series RLC circuit, for two values of R.
Fig 33-19b, p.1050

48. circuit increases. This signal caused by the incoming wave is then amplified and fed to
a speaker. Because many signals are often present over a range of frequencies, it is
important to design a high-Q circuit to eliminate unwanted signals. In this manner,
stations whose frequencies are near but not equal to the resonance frequency give
signals at the receiver that are negligibly small relative to the signal that matches the
resonance frequency.
Figure Average power versus frequency for a series RLC circuit. The width of each curve is measured between the two points where the power is half its maximum value. The power is a maximum at the resonance frequency 0.
Fig 33-20, p.1051

49. losses are reduced by using a laminated core
losses are reduced by using a laminated core. Iron is used as the core material because
it is a soft ferromagnetic substance and hence reduces hysteresis losses. Transformation
of energy to internal energy in the finite resistance of the coil wires is usually quite
small. Typical transformers have power efficiencies from 90% to 99%. In the discussion
Figure An ideal transformer consists of two coils wound on the same iron core. An alternating voltage  V1 is applied to the primary coil, and the output voltage  V2 is across the resistor of resistance R.
Fig 33-21, p.1052

50. Figure 33.22 Circuit diagram for a transformer.
Fig 33-22, p.1052

51. Nikola Tesla American Physicist (1856–1943) Tesla was born in Croatia but spent most of his professional life as an inventor in the United States. He was a key figure in the development of alternating-current electricity, high-voltage transformers, and the transport of electrical power using AC transmission lines. Tesla’s viewpoint was at odds with the ideas of Thomas Edison, who committed himself to the use of direct current in power transmission. Tesla’s AC approach won out. (UPI/CORBIS)
p.1053

52. Figure The primary winding in this transformer is directly attached to the prongs of the plug. The secondary winding is connected to the wire on the right, which runs to an electronic device. Many of these power-supply transformers also convert alternating current to direct current.
Fig 33-23, p.1053

53. This transformer is smaller than the one in the opening photograph for this chapter. In addition, it is a step-down transformer. It drops the voltage from V to 240 V for delivery to a group of residences.
p.1053

54. Figure (a) A half-wave rectifier with an optional filter capacitor. (b) Current versus time in the resistor. The solid curve represents the current with no filter capacitor, and the dashed curve is the current when the circuit includes the capacitor.
Fig 33-24, p.1055

55. Figure 33.24 (a) A half-wave rectifier with an optional filter capacitor.
Fig 33-24a, p.1055

56. Figure 33. 24 (b) Current versus time in the resistor
Figure (b) Current versus time in the resistor. The solid curve represents the current with no filter capacitor, and the dashed curve is the current when the circuit includes the capacitor.
Fig 33-24b, p.1055

57. Active Figure 33. 25 (a) A simple RC high-pass filter
Active Figure (a) A simple RC high-pass filter. (b) Ratio of output voltage to input voltage for an RC high-pass filter as a function of the angular frequency of the AC source.
Fig 33-25, p.1055

58. Active Figure 33.25 (a) A simple RC high-pass filter.
Fig 33-25a, p.1055

59. Active Figure (b) Ratio of output voltage to input voltage for an RC high-pass filter as a function of the angular frequency of the AC source.
Fig 33-25b, p.1055

60. Active Figure 33. 26 (a) A simple RC low-pass filter
Active Figure (a) A simple RC low-pass filter. (b) Ratio of output voltage to input voltage for an RC low-pass filter as a function of the angular frequency of the AC source.
Fig 33-26, p.1056

61. Active Figure 33.26 (a) A simple RC low-pass filter.
Fig 33-26a, p.1056

62. Active Figure (b) Ratio of output voltage to input voltage for an RC low-pass filter as a function of the angular frequency of the AC source.
Fig 33-26b, p.1056

63. Fig Q33-2, p.1058

64. Fig Q33-22, p.1058

65. Fig P33-3, p.1059

66. Fig P33-6, p.1059

67. Fig P33-7, p.1059

68. Fig P33-25, p.1060

69. Fig P33-26, p.1060

70. Fig P33-30, p.1061

71. Fig P33-36, p.1061

72. Fig P33-47, p.1062

73. Fig P33-55, p.1062

74. Fig P33-56, p.1062

75. Fig P33-58, p.1063

76. Fig P33-61, p.1063

77. Fig P33-62, p.1063

78. Fig P33-64, p.1063

79. Fig P33-69, p.1064

80. Fig P33-69a, p.1035

81. Fig P33-69b, p.1035

82. (* داخل الدوال المثلثية معطى بوحدة الراديان 1rad = 180o/π )
س ) وصلت دائرة RLC على التوالي مع مصدر للجهد المتردد = V vrms فوجد أن تيار الدائرة يعطى من العلاقه i(t) = 5.73 sin (377 t ) فإذا كان XL = 30 Ω and R = 20 Ωفإن:
(* داخل الدوال المثلثية معطى بوحدة الراديان 1rad = 180o/π )
Q27-32) A series RLC circuit connected to AC source of vrms = V and
i(t) = 5.73 sin (377 t ). If XL = 30 Ω and R = 20 Ω, then:
(*inside the sine is given in the unit of radian; 1rad = 180o /π )