Electrical Power and Machines Lecture 4 <Dr Ahmed El-Shenawy> <Dr Hadi El Helw> DC Generators Electric Equivalent Circuit of a DC Generator Field Winding Ra ia + E RL Field winding is responsible of setting up a flux Types of DC Generators 1. Permanent Magnet Generators φ Constant Flux Ra + E Ia Ia = IL IL RL This type is characterized by being smaller, lighter and more efficient compared to wound generators 2. Electro-magnet Generators a. Separately Excited Rf If + - Ia = IL b. VF Ia E Ra RL Self Excited IL Rf + Ia If E Ra Ia = If + IL RL IL Induced E.M.F Equation e.m.f “EC” is generated in armature windings EC = BLV N B: Flux density (T) L L: length of conductor (m) r V: velocity of conduction motion V =Wr B =φ / A = φ/ L Ap = φ/ [L(πD/P)] V = Wr = (2πN/60)r Then (N: rev/min) WD PW L L ( D P ) 2 2 Ec S Machine e.m.f “Ea” = EC (total no. of conductors/no. of parallel paths) Ea PW Z K a pW 2 a Where Ka = ZP/2 π a ……………….. Machine constant And Z = 2 C NC (C:no. of coils, NC : no. of turns) Example Calculate the voltage generated by a six pole dc machine if its windings are: 1) lap wound 2) Wave wound, if the flux per pole is 0.05 wb. and the generator speed is 120 rev/min, 200 armature coils with 15 turns each Solution Z = 2CNC = 2×200×15 = 6000 conductors 1)Lap wound a= P=6 Ea = Ka φp w = [6000×6/2π ×6]×0.05×[2π×120/60] = 600 V 2)Wave wound a=2 Ea = Ka φp w = [6000×6/2π×2]×0.05×[2π×120/60] = 1800 V Torque Equation P = Ea Ia = Ka φp w Ia = T × w Then the developed torque is given by: Td = P/w = Ka φp Ia Example A 24 slot, 2 pole Dc machine has 18 turns per coil, the average flux density per pole is 1T. The effective length is 20 cm and the armature radius is 10 cm. the magnetic poles are designed to cover 80 % of the armature periphery. If the armature velocity is 183.2 rad/sec and the armature current is 25 A, determine: • the current in each conductor • the developed torque • the developed power Solution •As the machine is a 2 pole, •then IC = Ia / 2 = 25/2 = 12.5 A • Ap = 2πrL/p = 2×3.14×0.1×0.2/2 = 0.063 m2, •as Ae = 0.8 Ap , •then Ae = 0.8×0.063 = 0.05 m2, •then φp = B Ae = 1×0.05 = 0.05 wb •and Ka = (Zp/2πa) = (2×24×18)×2/2П×2 = 137.51 •Td = Ka Ia φp = 137.51×25×0.05 = 171.89 N.m • Pd = Td ×w = 171.89×183.2 = 31490 W Magnetization characteristics of DC machine As Ea α φp w, now if the armature circuit is left open, and armature is rotated at rated speed, then Ea = K1 φp = Ka wm φp and since φp = Kf If (flux per pole depend on the Induced E.M.F at no load m.m.f provided by current If ) then Ea = K1 Kf If Since Ea is an indirect measure of the flux per pole and since If is a measure of the applied m.m.f (Nf If ), then the curve is similar to a B-H curve Air gap line Magnetic circuit Air gap m.m.f From previous operation of the machine Er Field Current If m.m.f required for magnetic material is almost negligible at small values of flux density Separately Excited Dc Generator VF Ea = Vt + Ia Ra IL = Ia Rf If + - Vf = If Rf Ia E Ra RL Ea = VN L - Vt IL + Drop due to armature resistance and reaction Vt Speed Shunt Generator Rf If = Vt /Rf Ia = IL +If Ia Vt = Ea – IaRa =ILRL If + E Ra Ia IL RL - Terminal Voltage VNL Er Magnetization curve el d Fi sis re ta e nc lin Vt + •Er induces an e.m.f in armature winding (Er) and as the field is parallel then a small If flows giving a m.m.f that sets up a flux giving aid to the residual flux. •An increase in the flux per pole will increase the induced e.m.f thus increasing If •The shunt generator continues to build up voltage until the point of intersection of the field resistance line and the magnetization saturation curve e If Note : A decrease in the field circuit resistance will cause the shunt generator to build up faster to a higher voltage, the generator will not build up if the field resistance is greater than or equal the critical resistance RF2 RC RF RF1 Terminal Voltage VNL Er RC >RF2 >RF >RF1 If Series Generator Rf Vt = Ea – Ia Ra –Ia Rf RL + TS Ea Vt Ia = IL = If IL - IL = Vt /RL + Ia Ra wm •Series generators are used to supply a constant load current •Rf should be small to reduce voltage drop (so it is made of thick wire) Voltage Regulation Voltage regulation is a measure of the terminal voltage drop at full load V.R % = 100×(VNL – VFL )/VFL VNL: NO load terminal voltage VFL : Full load terminal voltage Losses in DC Generators Input Mechanical Power Rotational losses “Pr” Mechanical Losses: • Windage (drag on armature caused by air) • Friction (brushes-commutator , bearing-shaft) Magnetic Losses: • Hysteresis losses • Eddy losses Developed Power “Pd” = EaIa • Output Power “Po” =Vt IL • Copper Losses “PCU” = I2R r P (R ot at io na l) Power Flow Diagram Pin = T SWm Pd =TdWm= EaIa P0 = Vt I L P CU = I2 R Efficiency “η” η %= (P0 /Pin) ×100 Example: The d.c Separately-excited generator shown in Fig produces an open circuit emf E of 220 V. Calculate the Terminal voltage V when generator supplies a current of 10 A. The armature resistance is 1 ohm Vt=Ea – Ra Ia Where Ea= 220 V Vt=220 – (10)(1) =210 V Ia= 10 A Ra= 1 ohm Example: A separately-excited d.c. generator produces an open-circuit voltage of 250 V with field current of 1.5 A. If the field current is increased to 2 A, calculate a) The new open-circuit emf. b) The terminal voltage if the generator supplies a current of 5 A. Assume armature resistance- 0.8 ohm and the speed remains constant. Solution: a) Since the speed is constant b) E1 I f 1 E2 If2 Where E1=250 V, If1= 1.5 A and If2 = 2A E2=250 (2/1.5)=333 V b) Vt=Ea – Ra Ia Where Ea=333 V, Ia= 5 A and Ra = o.8 ohm V= 333 – (5)(0.8) = 333 – 4 = 329 V Example A separately excited DC generator has a field resistance of 50 ohm, armature resistance of 0.125 ohm and brush drop of 2V. At no load the generated voltage is 275 V, and the full load current is 95 A. the field excitation voltage is 120 V and the friction windage and core losses are 1500 watt. Calculate : • The rated terminal voltage and output power • the efficiency at full load Solution VF Vt = Ea –IaRa –VB = 275-95×0.125-2 = 261.13 V P0 = Vt Ia = 26.13×95=24.81 Kw Rf If = 24.81×103+1500+952×0.125+1202/50 + - Pin = P0 + Plosses Ia E Ra RL = 27.913 Kw η = (24.81/27.913)×100 = 88.88 % - Vt IL +