Chapter 11 AC Circuit Power Analysis PDF

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DedicatedRhenium

Uploaded by DedicatedRhenium

2013

William H. Hayt, Jr., Jack E. Kemmerly, Steven M. Durbin

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AC circuit analysis electrical engineering power analysis power factor

Summary

This is an AC circuit power analysis chapter. It covers topics such as instantaneous power, average power, apparent power, complex power, reactive power, effective current and voltage values. The chapter also covers cases of maximum power transfer and power factor. An example about average power is shown.

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Chapter 11 AC Circuit Power Analysis Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for 1 reproduction or display. Objectives At the end of this chapter, you should be able to: 1. Compute real power, reactive power, apparent power, and/or power...

Chapter 11 AC Circuit Power Analysis Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for 1 reproduction or display. Objectives At the end of this chapter, you should be able to: 1. Compute real power, reactive power, apparent power, and/or power factor for a circuit or element. Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for rep 2 Introduction  This chapter examines different representations of power in an AC circuit.  These power representations include:  Instantaneous power  Average power  Apparent power  Complex power  Reactive power Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for rep 3 Introduction  In addition to these power representations, other related measures are defined.  These include:  Effective (RMS) current and voltage  Power factor Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for rep 4 Instantaneous Power The instantaneous power is p(t)=v(t)i(t). At all times t, power supplied = power absorbed Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 5 Power from Sinusoidal Source If in the same RL circuit, the source is Vmcos(ωt), then and so the power will be Double Constant Frequency Term Term Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 6 Average Power  The average power over an arbitrary interval from t1 to t2 is  When p(t) is periodic with period T, the average power is calculated over any one period: Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 7 Average Power: Sinusoidal Steady State If v(t)=Vmcos(ωt+θ) and i(t)=Imcos(ωt+ϕ), then 1 P  Vm I m cos(   ) 2  Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 8 Average Power for Elements  The average power absorbed by a resistor R is 2 1 1 2 V PR  Vm I m  I m R  m 2 2 2R  The average power absorbed by a purely reactive element(s) is zero, since the current and voltage are 90 degrees out of phase: PX 0 Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 9 Example: Average Power Find the average power being delivered to an impedance ZL= 8 − j11 Ω by a current I= 5ej20° A. Only the 8-Ω resistance enters the average-power calculation, since the j11-Ω component will not absorb any average power. Thus, P = (1/2)(52)8 = 100 W Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 10 Example: Average Power Find the average power absorbed by each element. Answer: PL=0 W PC=0 W, PR=25 W Pleft=-50 W Pright=25 W Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 11 Maximum Power Transfer  An independent voltage source in series with an impedance Zth delivers a maximum average power to a load impedance ZL which is the conjugate of Zth: ZL = Zth*  That is, if Z L RL  jX L & Z th Rth  jX th  Then, RL Rth X L  X th & Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 12 Maximum Power Transfer Derivation First, solve for the load power: 2 1 2| Vth | RL  2 2 (Rth  RL )  (X th  X L ) Clearly, P is largest when XL+Xth=0 Solving dP/dRL=0 will show that RL=Rth Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 13 Effective Values of Current and Voltage  Effective value of a periodic current (voltage) is equal to the value of the direct current (voltage) required to deliver the same average power to a resistor R.  The same power is delivered to the resistor in the circuits shown. periodic, period T Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 14 Effective Values of Current and Voltage  It can be shown the effective value of a current (voltage) is obtained by taking the square-root of the mean or average value of the square of the instantaneous current (voltage).  Effective value often called root-mean-square or rms value Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 15 Effective (RMS) for Sine Wave  For sine waves: V  1 eff Vm 0.707Vm 2 1 I eff  I m 0.707 I m 2  Average power can calculated using effective values 2 V P Veff I eff cos    P I R 2 eff P eff R Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 16 Apparent Power & Power Factor  Ifv(t)=Vmcos(ωt+θ) and i(t)=Imcos(ωt+ϕ), then 1 P  Vm I m cos(   ) Veff I eff cos(   ) 2  The apparent power is defined as VeffIeff and is given the units volt-ampere VA.  Apparent power is the power that would  apparently be absorbed if a load impedance behaved exactly like a resistor. Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 17 Apparent Power & Power Factor Power factor is defined as average power P PF   apparent power Veff I eff  fora resistive load, PF=1  fora purely reactive load, PF=0  generally, 0 ≤ PF ≤ 1  Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 18 Power Factor: Lagging & Leading  Since the power factor for sine waves is PF cos(   )  The information as to whether current leads or lags voltage is lost, so we add the adjective to the power factor term.  An inductive load has a lagging PF (I lags V).  A capacitive load has a leading PF (I leads V). Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 19 Example: Power Factor Find the average power delivered to each of the two loads, the apparent power supplied by the source, and the power factor of the combined loads. Answer: 288 W, 144 W, 720 VA, PF=0.6 (lagging) Copyright © 2013 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 20

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