fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
fundamentals of engineering supplied-reference handbook - Ventech!
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AC POWER<br />
Complex Power<br />
Real power P (watts) is defined by<br />
P = (½)VmaxImax cos θ<br />
= VrmsIrms cos θ<br />
where θ is the angle measured from V to I. If I leads (lags)<br />
V, then the power factor (p.f.),<br />
p.f. = cos θ<br />
is said to be a leading (lagging) p.f.<br />
Reactive power Q (vars) is defined by<br />
Q = (½)VmaxImax sin θ<br />
= VrmsIrms sin θ<br />
Complex power S (volt-amperes) is defined by<br />
S = VI* = P + jQ,<br />
where I* is the complex conjugate <strong>of</strong> the phasor current.<br />
S=VI<br />
θ<br />
P=VIcosθ<br />
Q=VIsin θ<br />
Complex Power Triangle (Inductive Load)<br />
For resistors, θ = 0, so the real power is<br />
P = V I =<br />
2<br />
V<br />
2<br />
/ R = I R<br />
rms rms rms rms<br />
Balanced Three-Phase (3-φ) Systems<br />
The 3-φ line-phase relations are<br />
for a delta<br />
for a wye<br />
VL = Vp<br />
V = 3V = 3V<br />
I = 3I<br />
IL = Ip<br />
L p<br />
L p LN<br />
where subscripts L/P denote line/phase respectively.<br />
A balanced 3-φ delta-connected load impedance can be<br />
converted to an equivalent wye-connect load impedance<br />
using the following relationship<br />
Z ∆ = 3Z Y<br />
The following formulas can be used to determine 3-φ power<br />
for balanced systems.<br />
S = P+ jQ<br />
S = 3VI = 3VI<br />
P P L L<br />
3 P<br />
*<br />
P<br />
3VI L Lcos P jsin<br />
P<br />
( )<br />
S= V I = θ + θ<br />
For balanced 3-φ wye- and delta-connected loads<br />
2<br />
= *<br />
L V<br />
S<br />
Z<br />
2<br />
L = 3 *<br />
V<br />
S<br />
Z<br />
Y<br />
∆<br />
171<br />
ELECTRICAL AND COMPUTER ENGINEERING (continued)<br />
where<br />
S = total 3-φ complex power (VA)<br />
S = total 3-φ apparent power (VA)<br />
P = total 3-φ real power (W)<br />
Q = total 3-φ reactive power (var)<br />
θ P = power factor angle <strong>of</strong> each phase<br />
V L = rms value <strong>of</strong> the line-to-line voltage<br />
V LN = rms value <strong>of</strong> the line-to-neutral voltage<br />
I L = rms value <strong>of</strong> the line current<br />
I P = rms value <strong>of</strong> the phase current<br />
For a 3-φ wye-connected source or load with line-to-neutral<br />
voltages<br />
Van<br />
= VP∠°<br />
0<br />
Vbn<br />
= VP∠−<br />
120°<br />
V = V ∠+ 120°<br />
cn P<br />
The corresponding line-to-line voltages are<br />
V<br />
V<br />
V<br />
= 3V∠ 30°<br />
ab P<br />
= 3V∠− 90°<br />
bc P<br />
= 3V∠+ 150°<br />
ca P<br />
Transformers (Ideal)<br />
Turns Ratio<br />
a = N1<br />
N2<br />
V p<br />
a =<br />
V<br />
=<br />
I<br />
I<br />
s<br />
The impedance seen at the input is<br />
ZP = a 2 ZS<br />
s<br />
p