This requires that the analysis be done in the time domain. For a Y - connected load, the phase voltages are
Van = √2 Vp coswt ,
Vbn = √2 Vp cos(wt - 120), Vcn =
√2 Vp cos(wt + 120)
where the factor √2 is important because Vp has been
defined as the rms value of the phase voltage. If Zy = Z∠Ɵ, the phase
currents lag behid their corresponding phase voltage by Ɵ.
ia = √2Ip cos(wt - Ɵ),
ib = √2Ip cos(wt - Ɵ -
120)
ib = √2Ip cos(wt - Ɵ + 120)
ib = √2Ip cos(wt - Ɵ + 120)
TOTAL INSTANTANEOUS POWER
p = pa + pb + pc = VANia + VBNib + VCNic
= 2VpIp [ coswt cos(wt - Ɵ) + cos(wt - 120) cos(wt - Ɵ - 120) + cos(wt + 120) cos(wt - Ɵ + 120) ]
p = 3VpIp cosƟ
INSTANTANEOUS POWER PER PHASE IS:
p = VpIp cosƟ
REACTIVE POWER PER PHASE IS:
Qp = VpIp sinƟ
APPARENT POWER PER PHASE IS:
Sp = VpIp
COMPLEX POWER PER PHASE IS :
Sp = Pp + jQp = Vp Ip*
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