VC 2π fr L 1 1 = = = V R 2π f r CR R fr Q= or f2 − f1 fr ( f2 − f 1) = Q
Current growth: v L = Ve−(Rt /L)
Current decay: v L = v R = V e−(Rt /L) i = I e−(Rt /L)
Single-phase circuits
Series resonance: fr =
L−R circuit
power factor = cos φ =
R Z
√ (P1 − P2 ) tan φ = 3 (P1 + P2 )
Copyrighted material - Taylor & Francis Main formulae for Part 2
V1 N1 I2 = = V2 N2 I1
I0 =
2 + I2) (I M C
I M = I0 sin φ0
IC = I0 cos φ0
E2 − E1 E = 4.44 f m N Regulation = × 100% E2 2 V1 Equivalent circuit: Re = R1 + R2 V2 2 V1 Xe = X1 + X2 V2 Z e = (Re2 + X e2 ) losses Efficiency, η = 1 − input power Output power = V2 I2 cos φ2 Total loss = copper loss + iron loss Input power =output power +losses 2 N1 Resistance matching: R1 = RL N2
D.c. machines General e.m.f. E =
2 pn Z ∝ ω c
(c = 2 for wave winding, c =2 p for lap winding)
Generator: E = V + Ia Ra
VI Efficiency, η = × 100% VI + Ia2 Ra + I f V + C E = V − I a Ra
Motor:
Efficiency, η =
VI − Ia2 Ra − I f V − C VI
Torque =
× 100%
pZIa EIa = ∝ Ia 2πn πc
Three-phase induction motors f ns = s= p
n s − nr ns
× 100
fr = s f
Xr = s X2
N2 s E1 I 2 R2 Er N1 s= r Ir = = Zr P2 [R22 + (s X 2 )2 ] Efficiency, η =
Pm Pl
input – stator loss – rotor copper loss – friction and windage loss = input power
s E 12 R2 m(N2 /N1 )2 Torque, T = 2πn s R22 + (s X 2 )2 ∝
s E 12 R2 R22 + (s X 2 )2
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