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AC Power Discussion D9.3 Chapter 5 Steady-State Power • • • • • • Instantaneous Power Average Power Effective or RMS Values Power Factor Complex Power Residential AC Power Circuits Instantaneous Power v(t ) VM cos t v i(t ) I M cos t i p(t ) v(t )i(t ) VM I M cos t v cos t i VM I M cos v i cos 2t v i p(t ) 2 Note twice the frequency Average Power T 2 1 P T t0 T t0 1 P T 1 p(t )dt T t0 T t0 t0 T t0 VM I M cos t v cos t i dt VM I M cos v i cos 2t v i dt 2 P 1 VM I M cos v i 2 Purely resistive circuit Purely reactive circuit v i 0 v i 90 P 1 VM I M 2 P 1 VM I M cos 90 0 2 Effective or RMS Values We define the effective or rms value of a periodic current (voltage) source to be the dc current (voltage) that delivers the same average power to a resistor. 1 PI R T 2 eff I eff t0 T t0 i 2 (t )Rdt 1 t0 T 2 i (t )dt T t0 I eff I rms Veff2 1 P R T t0 T t0 v 2 (t ) dt R 1 t0 T 2 Veff v (t )dt T t0 root-mean-square Veff Vrms Effective or RMS Values Vrms Using Vrms Vrms 1 t0 T 2 v (t )dt T t0 v(t ) VM cos t v cos 1 1 cos 2 2 2 2 VM 2 VM 2 2 0 2 0 T 2 and 1 1 cos 2t 2v dt 2 2 1 dt 2 1 2 VM 2 2 t 20 1 2 1 2 VM 2 Power Factor Recall Average Power Vrms VM 2 P 1 VM I M cos v i 2 IM I rms 2 P Vrms I rms cos v i Power factor P PF cos v i cos ZL Vrms I rms Power factor angle Note that I rms ZL v i P Vrms PF Thus, an industrial load that consumes P watts with a high PF from a Vrms volt 2 R line losses. line will have lower I rms Complex Power Complex Power S = Vrms Irms I rms complex conjugate of I rms rms I r jIi I rms i rms I r jI i I rms i S = Vrms v I rms i Vrms I rms v i S = P jQ P Re(S) Vrms I rms cos v i Real, average power Q Im(S) Vrms I rms sin v i Imaginary, quadrature power Residential Power Systems Read Section 5-8, pages 216 - 219