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Power flow and measurement

Written By Sajib Barua on Sunday, November 24, 2013 | 12:26 AM

Single-phase

Suppose we have a single-phase load as in Figure 2.7 supplied with a sinusoidal voltage whose instantaneous value is clip_image002[8]. The RMS value is clip_image004[6] and the phasor value is V. If the load is linear (i.e. its impedance is constant and does not depend on the current or voltage), the current will be sinusoidal too. It leads or lags the voltage by a phase angle clip_image006[4], depending on whether the load is capacitive or inductive. With a lagging (inductive) load, clip_image008[4] ; see Figure 2.29.

The instantaneous power is given by clip_image010[4], so

clip_image012[4] (2.30)

This expression has a constant term and a second term that oscillates at double frequency. The constant term represents the average power clip_image014[6]: we can write this as

clip_image002  (2.31)

clip_image014[7] is equal to the product of the rms voltage clip_image004[7], the RMS current clip_image018[4], and the power factor clip_image020[4]. The amplitude of the oscillatory term is fixed: i.e. it does not depend on the power factor. It shows that the instantaneous power clip_image022[4] varies from clip_image024[6] to clip_image026[4] and back to clip_image024[7] twice every cycle. Since the average power is VmIm/2, this represents a peak-peak fluctuation 200% of the mean power, at double frequency. The oscillation of power in single-phase circuits con- tributes to lamp flicker and causes vibration in motors and transformers, producing undesirable acoustic noise.

 

Instantaneous current, voltage and power in a single-phase AC circuit

Fig. 2.29  Instantaneous current, voltage and power in a single-phase AC circuit.

Two-phase

Suppose we have a two-phase load with phases a and b, with υa = Vm cos ωt, ia = Im cos (ωt – ϕ) and υb = Vm sin ωt, ib = Im sin (ωt - ϕ). This system is said to be balanced, because the voltages and currents have the same RMS (and peak) values in both phases, and their phase angles are orthogonal. The total instantaneous power is now given by

image

The oscillatory term has vanished altogether, which means that the power flow is constant, with no fluctuation, and the average power P is therefore equal to the instantaneous power p. Note that if the phases become unbalanced, an oscillatory term reappears.

Three-phase
Suppose we have a three-phase load as in Figures 2.20 and 2.22, with phases a, b and c, with

image

This system is said to be balanced, because the voltages and currents have the same RMS (and peak) values in all three phases, and their phase angles are equi-spaced (i.e. with a 120o symmetrical phase displacement). The total instantaneous power is now given by

image


As in the two-phase system, the oscillatory term has vanished. The power flow is constant, with no fluctuation, and the average power P is equal to the instantaneous power p. If the phases become unbalanced, an oscillatory term reappears.


The voltages and currents in equation (2.34) are phase quantities. In terms of line quantities, for a wye connection we have image  and IL = Iph, whereas for a delta connection we have image and VLL = Vph. In both cases, therefore,

image

where ϕ is the angle between the phasors Vph  and Iph.
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