电子电工技术英文课件 (33).pdf
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1、3.6 AC Power 3.6.1 Instantaneous Power In AC circuits,if the current of a resistor is m()cosi tIt=,its voltage will bem()()cosv tRi tRIt=.The instantaneous power of the resistor is 222mm(1cos2)()()()cos2RItp tv t i tRIt+=(1)The waveform of p(t)of the resistor is shown in Fig.1.Figure 1:Instantaneous
2、 power waveform of the resistor.If the current of an inductor is m()cosi tIt=,its voltage will be m()()sindi tv tLLItdt=.The instantaneous power of the inductor is 22mm()()()sincossin22LIp tv t i tLIttt=(2)The waveform of p(t)of the resistor is shown in Fig.2.Figure 2:Instantaneous power waveform of
3、 the inductor.In the same way,we can get the instantaneous power of a capacitor 2mmm1()()()sincossin22Ip tv t i tItIttCC=(3)The waveform of p(t)of the capacitor is shown in Fig.3.Figure 3:Instantaneous power waveform of the capacitor.From(1)-(3),the instantaneous power of AC circuits varies with tim
4、e periodically.Therefore,it is difficult to measure the power of AC circuits quantitatively by the instantaneous power.3.6.2 Average Power(Active Power)In order to measure the power of AC circuits quantitatively,the instantaneous power varying with time periodically can be averaged during a period T
5、 of sinusoidal voltage and current.av01()TPp t dtT=(4)The average value Pav of the instantaneous power is called average power or active power.For a resistor,from(1)and(4),the average power is 22mmRav0011(1cos2)()=22TTRItRIPp t dtdtTT+=(5)For an inductor,from(2)and(4),the average power is 2mLav0011(
6、)sin2=0 W2TTLIPp t dttdtTT=(6)For a capacitor,from(3)and(4),the average power is 2mCav0011()sin2=0 W2TTIPp t dttdtTTC=(7)From(6)and(7),the average power of the inductor and capacitor in AC circuits is zero.The expressions(5)-(7)show that in AC circuits the resistor consumes average power,while both
7、the inductor and the capacitor do not consume average power.For any branch in AC circuits,we can calculate its average power as ()mmavmm0011()cos()cos()=cos2TTviviV IPp t dtVtItdtTT=+(8)where vi is the phase difference between the branch voltage and branch current.For a resistor,0vi=.According to(8)
8、,the average power of the resistor is ()ommmmmmRavcoscos0222viV IV IV IP=(9)For an inductor,o90vi=.According to(8),the average power of the inductor is ()ommmmLavcoscos900 W22viV IV IP=(10)For a capacitor,o90vi=.According to(8),the average power of the capacitor is ()ommmmCavcoscos(90)0 W22viV IV IP
9、=(11)The expressions(9)-(11)are in accordance with the expressions(5)-(7).3.6.3 Reactive Power From(10)and(11),the inductor and capacitor do not consume average power.Although the inductor and capacitor do not consume average power,they keep absorbing and delivering power,as shown in Fig.2 and Fig.3
10、.In order to measure the ability of power throughput of AC circuits quantitatively,we need to introduce another important concept:reactive power Q.For any branch in AC circuits,its reactive power is ()mm=sin2viV IQ(12)Q has been given the unit volt-ampere reactive(VAR).For a resistor,according to(12
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