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FUNDAMENTAL OF ELECTRICAL POWER SYSTEMS (EE 270) Chapter 3 Basic Principles 1 Objectives • Review basic concepts and establish terminology and notation encountered in electric circuit theory. • Review phasors, instantaneous power, complex power, network equations and elementary aspects of balance threephase circuits. 2 Power System Network 3 Three-Phase Power Transformer 4 Sub-station 5 Distribution Transformer 6 Phasors • Sinusoidal voltage or current at constant frequency characterized by: – Phase angle – Maximum value Instantane ous Voltage : v(t ) Vmax cos(t v ) Instantane ous Current : i(t ) I max cos(t i ) 7 Phasors • The root-mean-square effective value • Let the rms value of Voltage: Current: Vm V 2 • And let Im I 2 V i 8 Power in Single Phase AC Circuit Assume a single phase sinusoidal source supplying a load. v(t) = instantaneous voltage i(t) = instantaneous current Find the instantaneous power p(t) 9 Power in Single Phase AC Circuit p(t ) v(t )i (t ) Vm I m cost v cost i . . . V I cos V I sin Use trigonometric identity cos A cos B 1 1 cos( A B) cos( A B) 2 2 10 Power in Single Phase AC Circuit p(t ) v(t )i (t ) Vm I m cost v cost i 11 Real Power • The average power, P is also referred as the active power or real power. • The power absorbed by the resistive component of the load. • Standard unit: Watt P V I cos 12 Reactive Power • The power absorbed by the reactive component of the load. • Standard unit: var (volt-ampere reactive) Q V I sin 13 Complex Power • The complex power, S is the product of voltage and the conjugate of the current. • Standard unit: VA (volt-ampere) S P jQ S P Q 2 2 14 Complex Power S VI * V v I i VI v i VI cos v i jVI sin v i VI cos jVI sin P jQ 15 Phasor Diagram Purely Resistive Load Q=0; S=P Purely Inductive Load P=0 V I i v Purely Capacitive Load P=0 I V i v 16 Phasor Diagram 17 Power Triangle Purely Inductive Load P=0, Q=+ve S Q P Purely Capacitive Load P Q S P=0, Q=-ve 18 Power Triangle 19 Impedance • Impedance of complex power is given by: 2 V Z * S 20 The Complex Power Balance • The sum of real and reactive power supplied by the source is equal to the sum of real and reactive powers transferred to the load. • Law of energy conservation S source Sload 21 The Complex Power Balance I I3 I2 I1 Z1 Z3 Z2 V S VI V I1 I 2 I 3 VI VI 2 VI * * * 1 * * 3 22 The Complex Power Balance Example: V 12000 Z1 60 j 0 I I1 I2 I3 Z1 V Z2 Z3 Z 2 6 j12 Z3 30 j 30 Total load complex power , S ? 23 Solution Current at each load: V 12000 20 j 0 A I1 60 j 0 Z1 V 12000 40 j80 A I2 6 j12 Z2 V 12000 20 j 20 A I3 Z 3 30 j 30 24 Solution Complex power absorbed at each load: S1 VI1* 120020 j 0 24kW S 2 VI 2 * 120040 j80 48kW j 96k var S3 VI 3 * 120020 j 20 24kW j 24k var Total load complex power: Stotal S1 S 2 S3 96kW 72k var 25 Exercise Two loads connected in parallel are supplied from a single-phase 240Vrms source. The two loads draw a total real power of 400kW at a power factor of 0.8 lagging. One of the loads draws 120kW at a power factor of 0.96 leading. Find the complex power of the other load. 26 Exercise Two impedances, Z1=0.8+j5.6Ω and Z2=8-j16Ω, and a single phase motor are connected in parallel across a 200Vrms, 60Hz supply. The motor draws 5kVA at 0.8 pf lagging. Find S1, S2 and S3 for the motor. 27 Power Factor Correction PF cos • PF = 1 } unity power factor • If PF<1, apparent power |S|>real power P • Current increase, cost of utility increase. • Major loads of the system should be near to unity power factor. 28 Power Factor Correction • Inductive load : lagging pf • Capacitive load : leading pf • How to fix PF? Capacitor is added to the system (inductive load). • PF is mostly considered in industrial consumers (using inductive load) and not in residential and small commercial since the power factor is near unity. 29 Power Factor Correction 30 Power Factor Correction 31 Exercise Two loads Z1=100+j0Ω and Z2=10+j20Ω are connected across a 200Vrms, 50Hz source. (a) Find the total real and reactive power, the power factor at the load, and the total current without C. 200V (b) Find the capacitance of the capacitor connected across the loads to improve the overall power factor to 0.8 lagging. I I1 100 I2 Ic 10 j 20 C 32 Solution (a) Current at each load: Power at each load: 2000 I1 20 A 100 2000 I2 8.945 63.43 A 10 j 20 S1 VI1* 200020 4000VA S 2 VI 2 * 20008.94563.43 1.78963.43kVA 33 Solution (a) Total real and reactive power: S S1 S 2 4000 178963.43 400 800 j1600 1200 j1600VA P 1200W Q 1600 var Total current without C: S * 1200 j1600 I 10 53.13 A V* 2000 Power factor at the load: PF cos cos53.13 0.6 lagging 34 Solution (b) Power at the capacitor: P 1200Watt new cos 0.8 36.87 Qnew P tan new 1 1200 tan 36.87 900 var QC Q prev Qnew 1600 900 700 var 35 Solution (b) Capacitance of the capacitor: 2 SC VI C * V ZC * 2 200 2 ZC j 57.14 SC * j 700 V 1 1 C 55.7 F 2fZC 2 5057.14 36 Exercise Three loads are connected in parallel across a 1400Vrms, 50Hz single-phase supply. • • • Load 1: Inductive load, 125kVA at 0.28 power factor Load 2: Capacitive load, 10kW and 40kvar Load 3: Resistive load of 15kW (a) Find the total kW, kvar, kVA and the supply power factor. (b) A capacitor of negligible resistance is connected in parallel with the above loads to improve the power factor to 0.8 lagging. Determine the kvar rating of this capacitor and the capacitance in µF. 37 Exercise Two loads are connected in parallel across a 200Vrms, 50Hz single-phase supply. • • Load 1: 0.8 + j5.6Ω Load 2: 8 - j16Ω (a) Find the total kW, kvar, kVA and the supply power factor. (b) A capacitor is connected in parallel with the loads. Find the kvar and the capacitance in µF to improve the overall power factor to unity. (c) What is the new line current? 38 Complex Power Flow • Need to consider two way current (i.e. From V1 to V2 and from V2 to V1) and two way S (i.e. From V1 to V2 and from V2 to V1). • If P is negative than the P in which the source is associated to receives/absorbs the P. • If P is positive than the P in which the source is associated to generates/delivers the P. • If Q is negative than the Q in which the source is associated to receives/absorbs the Q. • If Q is positive than the Q in which the source is associated to generates/delivers the Q. 39 Generator & Load Convention Convention P/Q Characteristic + Delivered/ Generated – Absorbed/ Received + Absorbed/ Received – Delivered/ Generated I + Vsource Generator Convention – I + Vload Load Convention – 40 Exercise Consider two voltage sources V1=120∟–5°V and V2=100∟0°V are connected by a short line of impedance Z=1+j7Ω. Determined the real and reactive power supplied or received by each source and the power loss in the line. I12 V1 Zshort line V2 41 Solution Find current which flows from V1 to V2 i.e. I12 V1 V2 120 5 1000 I12 3.135 110.02 A Z 1 j7 Find current which flows from V2 to V1 i.e. I21 V2 V1 1000 120 5 I 21 3.13569.98 A Z 1 j7 Find S from V1 to V2 i.e. S12 S12 V1I12 120 5 3.135110.02 376.2105.02 * Find S from V2 to V1 i.e. S21 S21 V I * 2 21 1000 3.135 69.98 313.5 69.98 42 Solution Evaluate the source from the previous calculated S. Based on S1: S12 376.2105.02 97.5W j363.3var Source 1 receive 97.5W and delivers 363.3var. Based on S2 S21 313.5 69.98 107.3W j 294.5var Source 2 generates 107.3W and receives 294.5var. 43 Solution Power loss in the line S L S12 S 21 97.5 j 363.3 107.3 j 294.5 9.8W j 68.8 var Check! PL R I12 1 3.135 9.8W 2 2 QL X I12 7 3.135 68.8 var 2 2 Thus, the real power loss in the line is 9.8W and the reactive power loss in the line is 68.6var. 44 Exercise Two single-phase ideal voltage sources are connected by a line of impedance of 0.7+j2.4Ω. V1=500∟16.26°V and V2=585∟0°V. Find the complex power for each source and determine whether they are delivering or receiving real and reactive power. Also, find the real and the reactive power loss in the line. 45 Review.. • Power in single-phase AC – S, P, Q, p(t) – Phasor analysis/diagram – Power triangle • Complex power balance • Power factor correction • Complex power flow – Generator / Load Convention 46