BEF BEF Chapter 2. Outline BASIC PRINCIPLES 09/10/2013. Introduction. Phasor Representation. Complex Power Triangle.

Size: px
Start display at page:

Download "BEF BEF Chapter 2. Outline BASIC PRINCIPLES 09/10/2013. Introduction. Phasor Representation. Complex Power Triangle."

Transcription

1 BEF 5503 BEF 5503 Chapter BASC PRNCPLES Outline ntroduction Phasor Representation Coplex Power Triangle Power Factor Coplex Power in AC Single Phase Circuits Coplex Power in Balanced Three-Phase Circuits One-line Diagra pedance Diagra Per Unit Analysis 1

2 ntroduction Power Concepts Per Unit Analysis Basic Principles of Power Systes Coplex Power Power Representations ntroduction R C L Power Syste Loads

3 ntroduction Tie Doain versus Frequency Doain Tie Doain: X M cost Frequency Doain: X X M ntroduction Sinusoids Period: T Tie necessary to go through one cycle Frequency: f = 1/T Cycles per second (Hz) Angular frequency (rads/sec): = f Aplitude: V M 3

4 ntroduction What is the aplitude, period, frequency, and angular (radian) frequency of this sinusoid? ntroduction Coplex Nuber aginary axis y x Real axis x is the real part y is the iaginary part z is the agnitude is the phase Polar Coordinates: A = z q Rectangular Coordinates: A = x + jy x z cos z x y y z sin y tan 1 x 4

5 ntroduction There is a good chance that your calculator will convert fro rectangular to polar, and fro polar to rectangular. Convert to polar: 3 + j4 and -3 - j4 Convert to rectangular: 45 & - 45 ntroduction Eleent Tie doain Phasor doain Resistance v = ir V = R Reactance v = L (di/dt) V = jl = jx Capacitance i = C (dv/dt) = jcv = jbv 5

6 ntroduction Phasor Representation The AC voltages and currents appearing in power systes can be represented by phasors, a concept useful in obtaining analytical solutions to one-phase and three-phase syste design. Phasor is generally defined as a transfor of sinusoidal functions fro the tie doain into the coplex-nuber doain. A phasor is a coplex nuber that contains the agnitude and phase angle inforation of a sinusoidal function. 6

7 Phasor Representation The Euler s identity that relates the exponential function to the trigonoetric functions is given as follows: j cos Re e e j cos j sin j sin e A sinusoidal voltage quantity v(t), with angular speed of ω rad/s, axiu voltage of V, and phase displaceent of θ 1 canbewrittenas: jt t Re V e v( t) V cos 1 1 j V e e j Re t 1 Phasor Representation Since the frequency is fixed in power studies, factor e jωt is equals to 1 and v(t) can be rewritten as: j1 v( t) V cost V e or 1 V 1 The instantaneous voltages and currents is not particularly concerned in power studies but ore with their RMS agnitudes and phase angles. V V j1 e V 1 j e Voltage Current Polar for 7

8 Phasor Representation The representation of RMS voltage and RMS current phasors in rectangular (or Cartesian) for are as follows: V VRMS cos1 j sin1 RMS cos j sin Coplex Power Triangle The coplex power (S in kva) is defined as a coplex nuber with the real part represents active power (P in kw) and the iaginary part represents reactive power (Q in kvar). S P jq Q L or Q C 8

9 Coplex Power Triangle S P Q L Power triangle for inductive loads P S Q C Power triangle for capacitive loads Coplex Power Triangle Exaple.1: Draw the power triangle for the following circuit: 9

10 Coplex Power Triangle Exaple.: Draw the power triangle for the following circuit: Power Factor Most of the loads in power syste are inductive type. For exaple: otors require REACTVE power (Q) to set up the agnetic field, and ACTVE power (P) to produce the useful work (shaft Horse Power). (Power Factor Angle) ACTVE power (P) REACTVE power (Q) 10

11 Power Factor Power Factor is a easure of how efficiently electrical power is consued. 100% of the energy burned is being used to ove the runner fro AtoB. Say, =30, only 87% of the energy burned is being used to ove the runner in the horizontal direction of B, and so extra energy will be required to achieve the sae objective. Power Factor Power Factor is the ratio of Active Power (P) to Apparent/ Total Power (S): (Power Factor Angle) ACTVE power (P) REACTVE power (Q) Power Factor Q tan P P(kW) S(kVA) cos Lagging (nductive Loads) Leading (Capacitive Loads) 11

12 Power Factor pact of poor power factor: Poor PF causes ore power losses Wasted Power Power Factor Exaple.3: An installation supplies the following loads: 10 kw at unity power factor; 15 kva at 0.8 p.f. lagging; 4 kvar leading. Calculate the total kw, kvar, the overall kva and power factor. [Ans. kw, 5 kvar (lag),.56 kva, (lag)] 1

13 Coplex Power in AC Single Phase Circuits To study steady-state behavior of circuits, consider the following sinusoidal voltage and current: v( t) V cost i t ) cos t Note that the current lags the ( voltage by an angle. The instantaneous power is defined as: p ( t ) vt i ( t ) p( t) V p V cos( t) cos( t ) cos cos t 1 ( ) cos cos t cos cos Coplex Power in AC Single Phase Circuits 13

14 Coplex Power in AC Single Phase Circuits V p( t) cos cos t A ore useful quantity is the average power that is being delivered. By averaging the instantaneous power over a specified tie-period, typically for one cycle, the average power, P, becoes: 0 V P cos cost V cos RMS RMS V cos V V ; RMS RMS Coplex Power in AC Single Phase Circuits Lagging power factor eans the current lags the voltage by an angle. Leading power factor eans the current leads the voltage by an angle. Lagging power factor Leading power factor 14

15 Coplex Power in AC Single Phase Circuits t is coon in electric power studies to set the voltage angle as the angular reference. The coplex power or the apparent power, S is defined as the product of voltage ties the conjugate of current, S V * V S V cos jv sin P V cos (W) Q V sin (VAr) S P jq POWER FACTOR cos costan 1 Q P P P Q P S Coplex Power in AC Single Phase Circuits Exaple.4: Consider the following 50 Hz based circuit with the given paraeters: 15

16 Coplex Power in AC Single Phase Circuits Exaple.4 (Cont.): Find the following: a) the source current, b) the active, reactive, and apparent power into the circuit, c) the power factor of the circuit. Coplex Power in AC Single Phase Circuits Solution.4: a) source current V 1000V 1 R jl 0.5 j rad / sec.110 V S 3 H 3 jc1000v j314.16rad / sec F b) power flows A A A A A 1 S V * c) power factor 1000V A j4573.1va P 700.5W Q VAr 3.4 PF cos(3.4) 0.84 lagging VA 16

17 Coplex Power in Balanced Three-Phase Circuits The ajor assuption of all the electric power presently used is generated, transitted, and distributed using balanced three-phase voltage systes. Three-phase operation is preferable to single-phase because a three-phase syste is ore efficient than a singlephase syste, and the flow of power is constant. Coplex Power in Balanced Three-Phase Circuits A balanced three-phase voltage syste is coposed of three single phase voltage sources having the sae agnitude and frequency but tie-displaced fro one another by 10 of a cycle as shown in the phasor diagras below: 17

18 Coplex Power in Balanced Three-Phase Circuits i A (t) V A (t) + V A =V0 Z Z = Z - V A (t)= V sint i B (t) V B (t) + V B =V-10 Z Z = Z - V B (t)= V sin(t-10 ) Current in three phases A B C V0 Z V Z V Z i C (t) V C (t) + V C =V-40 Z Z = Z - V C (t)= V sin(t-40 ) Coplex Power in Balanced Three-Phase Circuits A C B A Loads f three loads balanced, N = A + B + C = 0 B N C 18

19 Coplex Power in Balanced Three-Phase Circuits There are two possible connections of loads and sources in three-phase systes: wye-connection delta-connection Coplex Power in Balanced Three-Phase Circuits Wye (Y) and Delta () Connections a a V an n V bn V ab ca ab a a V cn b V bc b V ca V ca bc V bc V ab b c b c c c Wye (Y) Connection Delta () Connection 19

20 Coplex Power in Balanced Three-Phase Circuits Voltages and currents in Y connection: Van V V bn cn 0 V V V V LL = 3 V L = V ab V V an V V bn V V j V 3 1 3V j 3 V 30 Line voltage leads phase voltage by 30 Coplex Power in Balanced Three-Phase Circuits Phasor diagra for voltages in Y connection: 0

21 1 Voltages and currents in connection: Coplex Power in Balanced Three-Phase Circuits a c b c b a j j ca ab a L = 3 V LL = V Line current lags phase current by j Phasor diagra for currents in connection: Coplex Power in Balanced Three-Phase Circuits

22 Coplex Power in Balanced Three-Phase Circuits Power Relationships: Assue that a balanced three-phase voltage source is supplying a balanced load. The three sinusoidal phase voltages and currents can be written as: V V V a ( t) V sint a ( t) sint b( t) V sint 10 b( t) sint 10 b( t) V sint 10 ( t) sint 10 b Coplex Power in Balanced Three-Phase Circuits The three-phase power can be defined as: P3 V cos V cos V cos a a b b n trigonoetric identity, we get the following: P3 V 3cos cost cost 40 cost 40 The suation of the last three ters, in the above equation, is zero. Thus the three-phase power can be obtained as: P 3V cos 3 c c n phase quantities P3 3 V L L cos n line quantities

23 Coplex Power in Balanced Three-Phase Circuits Coplex Power The above analysis can be extended to include the reactive power, Q, or to get the apparent power, S, for a three-phase syste. S * * 3 3V 3 VL L f V V 0 and, then, S 3 3V 3V P 3 jq cos 3 j sin P 3 Q 3 3V 3V cos sin 3V L 3V L L L cos sin Coplex Power in Balanced Three-Phase Circuits Exaple.5: A wye-connected, balanced three-phase load consisting of three ipedances of 1030 is supplied with a balanced set of line-to-neutral voltages: V V an bn V cn 0V0 0V40 0VV 10 3

24 Coplex Power in Balanced Three-Phase Circuits Exaple.5: a) Calculate the phasor currents in each line, b) Calculate the line-to-line phasor voltages and show the corresponding phasor diagra c) Calculate the apparent power, active power, and reactive power supplied to the load Coplex Power in Balanced Three-Phase Circuits Solution.5: a) The phase currents of the loads are obtained as: an bn cn 00V 30A V 10A V A

25 Coplex Power in Balanced Three-Phase Circuits b) The line voltages are obtained as: V ab Or V V V ab bc ca V V 00V 040V 3 030V a b 3 V 3 V 3 V an bn cn Coplex Power in Balanced Three-Phase Circuits Relation between Phase and Line Voltages in a Wye-Connection: 5

26 Coplex Power in Balanced Three-Phase Circuits c) The powers are given by: * S3 3V 3Van P Q * an 00V 30A VA W 760.0VAr j760.0va One-line Diagra R Y B 3-phase syste one-line representation One-line diagra is a siplified single-line circuit diagra of a balanced three-phase electric power syste. t is indicated by a single line with standard apparatus sybols. 6

27 One-line Diagra Apparatus Sybols of One-line Diagra Or Machine or rotating arature Or Two-winding power transforer Or Three-winding power transforer Or Load Power circuit breaker, oil/ liquid Air circuit breaker Cont One-line Diagra Apparatus Sybols of One-line Diagra Busbar Three-phase, three- wire delta connection Transission line Three-phase wye, neutral ungrounded Fuse Current transforer A Three-phase wye, neutral grounded Aeter Or Potential transforer V Volteter 7

28 One-line Diagra One-line Diagra The inforation on a one-line diagra is vary according to the proble at hand and the practice of the particular copany preparing the diagra. Load/ Power Flow Study Transient Stability Study One-line Diagra Advantages of One-line Diagra Siplicity. One phase represents all three phases of the balanced syste. The equivalent circuits of the coponents are replaced by their standard sybols. The copletion of the circuit through the neutral is oitted. 8

29 One-line Diagra Exaple of one-line diagra (39-bus New England syste) One-line Diagra Exaple of one-line diagra (PSCAD/EMTDC) A SMPLE AC SYSTEM RRL #1 # s T FLAT30 Brk1 Vload [oh] C->G Flt1 ent (ka) Curre Voltage (kv) 3 Phase Source Current Phase Load Voltage 9

30 One-line Diagra Exaple of one-line diagra (PSCAD/EMTDC) NDUCTON MACHN NE WND FARM - ES [H] Use this coponent to study a wind gust or a rap and see the response of the control systes. ES Wind Source Mean w 1.0 A B Ctrl Pi Vw Ctrl = 1 CNT * 50.0 P Vw Actual hub speed of achine * * -1 N 3.0 Pole pairs 0.7 A B N/D D Ctrl Ctrl = 1 M wind gen Vw W A six Pole Machine Mechanical speed = W(pu)**pi*f/(pole paris) Pg W S T Beta * -1 The convention for the nduction achine is that input echanical torque is negative. (ie. otoring ode is positive) Wind Turbine MOD Type Beta BETA Wind Turbine Governor MOD Type T P TME TME CNT pedance Diagra pedance and Reactance Diagras pedance (Z = R + jx) diagra is converted fro oneline diagra showing the equivalent circuit of each coponent of the syste. t is needed in order to calculate the perforance of a syste under load conditions (Load flow studies) or upon the occurrence of a short circuit (fault analysis studies). Reactance (jx) diagra is further siplified fro ipedance diagra by oitting all static loads, all resistances, the agnetizing current of each transforer, and the capacitance of the transission line. t is apply to fault calculations only, and not to load flow studies. pedance and reactance diagras soeties called the Positive-sequence diagra. 30

31 pedance Diagra One-line diagra of an electric power syste pedance Diagra pedance diagra corresponding to the one-line diagra 31

32 pedance Diagra Reactance diagra corresponding to the one-line diagra E1 E E3 Generators 1 and Transforer T1 Transission Transforer Line T Gen. 3 Per Unit Analysis Coon quantities used in power syste analysis are voltage (kv), current (ka), voltaperes (kva or MVA), and ipedance (Ω). t is very cubersoe to convert currents to a different voltage level in a power syste having two or ore voltage levels. Per-unit representation is introduced such that the various physical quantities are expressed as a decial fraction or ultiples of base quantities and is defined as: actual quantity Quantity in per - unit base value of quantity 3

33 Per Unit Analysis Exaple.6: For instance, if a base voltage of 75 kv is chosen, actual voltages of 47.5 kv, 75 kv, and kv becoe 0.90, 1.00, and 1.05 per-unit, respectively. For siplicity, per-unit is always written as pu. For single-phase systes: Base current, A base kva 1 base voltage, kv base voltage, V Base ipedance base current, A Base power, kw 1 Base power, MW 1 base kva 1 base MVA 1 LN LN (base voltage, kv Base ipedance base kva 1 LN ) Per Unit Analysis For three-phase systes: Base current, A Base power, kw 3 Base power, MW 3 base MVA 3 3 X base voltage, kv (base voltage, kv Base ipedance base MVA base kva 3 base MVA 3 3 LL ) LL 33

34 Per Unit Analysis Exaple of power flow data in PU (39-bus New England syste) Per Unit Analysis Exaple.7: A three-phase, wye-connected syste is rated at 100 MVA and 13 kv. Express 80 MVA of three-phase apparent power as a per-unit value referred to (a) the three-phase syste MVA as base and (b) the single-phase syste MVA as base. Solution.7: (a) For the three-phase base, Base MVA = 100 MVA = 1 pu Base kv = 13 kv (LL) = 1 pu Per-unit MVA = 80/100 = 0.8 pu (b) For the single-phase base, Base MVA = 1/3 X 100 MVA = MVA = 1 pu Base kv = 13/ 3 = 76.1 kv = 1 pu Per-unit MVA = 1/3 X 80/ = 0.8 pu 34

35 Per Unit Analysis Changing the Base of Per-unit Quantities The ipedance of individual generators and transforers are generally in ters of % or pu quantities based on their own ratings (By anufacturer). For power syste analysis, all ipedances ust be expressed in pu on a coon syste base. Thus,it is necessary to convert the pu ipedances fro one base to another (coon base, for exaple: 100 MVA). Per-unit ipedance of a circuit eleent (actual ipedance, ) X (base MVA) (base voltage, kv) Per Unit Analysis The equation shows that pu ipedance is directly proportional to base MVA and inversely proportional p to the square of the base voltage. Therefore, to change fro old base pu ipedance to new base pu ipedance, the following equation applies: Per - unit Z new per - unit Z old base kv base kv old new base MVA base MVA new old 35

36 Per Unit Analysis Exaple.8: The reactance X of a generator is given as 0.0 pu based on the generator s naeplate rating of 13. kv, 30 MVA. The base for calculations is 13.8 kv, 50 MVA. Find X on this new base. Solution.8: x" pu Per Unit Analysis Exaple.9: A 30 MVA 13.8 kv three-phase generator has a subtransient reactance of 15%. The generator supplies two otors over a transission line having transforers at both ends, as shown in the one-line diagra below. The otors have rated inputs of 0 MVA and 10 MVA, both 1.5 kv with x = 0%. The three-phase transforer T1 is rated at 35 MVA, Y kv with leakage reactance of 10%. Transforer T is coposed of three single-phase transforers each rated at 10 MVA, Y kv with leakage reactance of 10%. Series reactance of the transission line is 80 Ω. Draw the reactance diagra with all reactances arked in per unit. Select the generator rating as base in the generator circuit. 36

37 Per Unit Analysis Solution.9: The three-phase rating of transforer T is 3 X 10 MVA = 30 MVA. ts line-to-line voltage ratio is X 67 = kv. A base of 30 MVA, 13.8 kv in the generator circuit requires a 30 MVA base in all parts of the syste and the following voltage bases: n transission line: 13.8(115/13.) = 10. kv. n otor circuit: 10.(1.5/116) = 13 kv. The reactances of the transforers converted to the proper base are: Transforer T1:X = 0.1 (13./13.8) (30/35) = pu. Transforer T:X =01(15/13) 0.1(1.5/13) = pu. The base ipedance of the transission line is (10. kv) /30 MVA = Ω and the reactance of the line is (80/481.6) = pu. Reactance of otor 1 = 0. (1.5/13) (30/0) = 0.77 pu. Reactance of otor = 0. (1.5/13) (30/10) = pu. Per Unit Analysis Solution.9: Reactance diagra: 37

38 Per Unit Analysis Exaple.10: Prepare an ipedance diagra of the given power syste. Show all the ipedances and source voltages in p.u. on a 100 MVA, 13 kv base in the transission line circuit. The necessary data for this syste are as follows: G1 : 50 MVA, 1. kv, X = 0.15 p.u. G : 0 MVA, 13.8 kv, X = 0.15 p.u. T1 : 80 MVA, 1./ 161 kv, X = 0.10 p.u. T : 40 MVA, 13.8/ 161 kv, X = 0.10 p.u. Load : 50 MVA, 0.80 power factor lagging, operating at 154 kv. Load odeled as a parallel cobination of resistance and inductance. Per Unit Analysis One-line diagra of the given power syste: (40 + j160) (0 + j80) (0 + j80) 38

39 Per Unit Analysis Solution.10: MVA base = 100 MVA. kv base: At transission line: 13 kv At G1 circuit : At G circuit : X13 kv kv. X13 kv kv. Per Unit Analysis pedance in p.u.: X pu(g1) = X pu(g) = X pu(t1) = p ( ) X pu(t) = j0.15 X j pu p.u j0.15 X j p.u j0.10 X j p.u j0.10 X j p.u

40 Per Unit Analysis pedance base at transission line circuit: Z base(tline) = Z pu(tline AB) = (13 kv) MVA 40 j j p.u Z pu(tline AC) = Z pu(tline BC) = 0 j j p.u Per Unit Analysis Load: 50 MVA (0.8 + j0.6) = (40 + j30) MVA R = X L = (154 kv) 40 MW (154 kv) 30 MVar R pu = X Lpu = p.u p.u

41 Per Unit Analysis Sources: E G1 pu = = 1./10.00 = 1. p.u. E G pu = = 13.8/ = 1. pu p.u. Per Unit Analysis pedance diagra: j pu j pu j pu j pu j pu j pu j pu 1. pu pu j4.537 pu 1. pu 41

Chapter 10 Objectives

Chapter 10 Objectives Chapter 10 Engr8 Circuit Analysis Dr Curtis Nelson Chapter 10 Objectives Understand the following AC power concepts: Instantaneous power; Average power; Root Mean Squared (RMS) value; Reactive power; Coplex

More information

Chapter 10 ACSS Power

Chapter 10 ACSS Power Objectives: Power concepts: instantaneous power, average power, reactive power, coplex power, power factor Relationships aong power concepts the power triangle Balancing power in AC circuits Condition

More information

Chapter 28: Alternating Current

Chapter 28: Alternating Current hapter 8: Alternating urrent Phasors and Alternating urrents Alternating current (A current) urrent which varies sinusoidally in tie is called alternating current (A) as opposed to direct current (D).

More information

ELG3311: Assignment 3

ELG3311: Assignment 3 LG33: ssignent 3 roble 6-: The Y-connected synchronous otor whose naeplate is shown in Figure 6- has a perunit synchronous reactance of 0.9 and a per-unit resistance of 0.0. (a What is the rated input

More information

ECE 420. Review of Three Phase Circuits. Copyright by Chanan Singh, Panida Jirutitijaroen, and Hangtian Lei, For educational use only-not for sale.

ECE 420. Review of Three Phase Circuits. Copyright by Chanan Singh, Panida Jirutitijaroen, and Hangtian Lei, For educational use only-not for sale. ECE 40 Review of Three Phase Circuits Outline Phasor Complex power Power factor Balanced 3Ф circuit Read Appendix A Phasors and in steady state are sinusoidal functions with constant frequency 5 0 15 10

More information

Chapter 10: Sinusoidal Steady-State Analysis

Chapter 10: Sinusoidal Steady-State Analysis Chapter 0: Sinusoidal Steady-State Analysis Sinusoidal Sources If a circuit is driven by a sinusoidal source, after 5 tie constants, the circuit reaches a steady-state (reeber the RC lab with t = τ). Consequently,

More information

PH 222-2C Fall Electromagnetic Oscillations and Alternating Current. Lectures 18-19

PH 222-2C Fall Electromagnetic Oscillations and Alternating Current. Lectures 18-19 H - Fall 0 Electroagnetic Oscillations and Alternating urrent ectures 8-9 hapter 3 (Halliday/esnick/Walker, Fundaentals of hysics 8 th edition) hapter 3 Electroagnetic Oscillations and Alternating urrent

More information

Chapter 10: Sinusoidal Steady-State Analysis

Chapter 10: Sinusoidal Steady-State Analysis Chapter 0: Sinusoidal Steady-State Analysis Sinusoidal Sources If a circuit is driven by a sinusoidal source, after 5 tie constants, the circuit reaches a steady-state (reeber the RC lab with t τ). Consequently,

More information

Fault Analysis Power System Representation

Fault Analysis Power System Representation .1. Power System Representation Single Line Diagram: Almost all modern power systems are three phase systems with the phases of equal magnitude and equal phase difference (i.e., 10 o ). These three phase

More information

Three Phase Circuits

Three Phase Circuits Amin Electronics and Electrical Communications Engineering Department (EECE) Cairo University elc.n102.eng@gmail.com http://scholar.cu.edu.eg/refky/ OUTLINE Previously on ELCN102 Three Phase Circuits Balanced

More information

Lecture (5) Power Factor,threephase circuits, and Per Unit Calculations

Lecture (5) Power Factor,threephase circuits, and Per Unit Calculations Lecture (5) Power Factor,threephase circuits, and Per Unit Calculations 5-1 Repeating the Example on Power Factor Correction (Given last Class) P? Q? S? Light Motor From source 1000 volts @ 60 Htz 10kW

More information

Lecture 2 Introduction

Lecture 2 Introduction EE 333 POWER SYSTEMS ENGNEERNG Lecture 2 ntroduction Dr. Lei Wu Departent of Electrical and Coputer Engineering Clarkson University Resilient Underground Microgrid in Potsda, NY Funded by NYSERDAR + National

More information

EEE3405 ELECTRICAL ENGINEERING PRINCIPLES 2 - TEST

EEE3405 ELECTRICAL ENGINEERING PRINCIPLES 2 - TEST ATTEMPT ALL QUESTIONS (EACH QUESTION 20 Marks, FULL MAKS = 60) Given v 1 = 100 sin(100πt+π/6) (i) Find the MS, period and the frequency of v 1 (ii) If v 2 =75sin(100πt-π/10) find V 1, V 2, 2V 1 -V 2 (phasor)

More information

ECEN 460 Exam 1 Fall 2018

ECEN 460 Exam 1 Fall 2018 ECEN 460 Exam 1 Fall 2018 Name: KEY UIN: Section: Score: Part 1 / 40 Part 2 / 0 Part / 0 Total / 100 This exam is 75 minutes, closed-book, closed-notes. A standard calculator and one 8.5 x11 note sheet

More information

ECE 421/521 Electric Energy Systems Power Systems Analysis I 2 Basic Principles. Instructor: Kai Sun Fall 2013

ECE 421/521 Electric Energy Systems Power Systems Analysis I 2 Basic Principles. Instructor: Kai Sun Fall 2013 ECE 41/51 Electric Energy Systems Power Systems Analysis I Basic Principles Instructor: Kai Sun Fall 013 1 Outline Power in a 1-phase AC circuit Complex power Balanced 3-phase circuit Single Phase AC System

More information

ECE 325 Electric Energy System Components 7- Synchronous Machines. Instructor: Kai Sun Fall 2015

ECE 325 Electric Energy System Components 7- Synchronous Machines. Instructor: Kai Sun Fall 2015 ECE 325 Electric Energy System Components 7- Synchronous Machines Instructor: Kai Sun Fall 2015 1 Content (Materials are from Chapters 16-17) Synchronous Generators Synchronous Motors 2 Synchronous Generators

More information

LO 1: Three Phase Circuits

LO 1: Three Phase Circuits Course: EEL 2043 Principles of Electric Machines Class Instructor: Dr. Haris M. Khalid Email: hkhalid@hct.ac.ae Webpage: www.harismkhalid.com LO 1: Three Phase Circuits Three Phase AC System Three phase

More information

EE221 - Practice for the Midterm Exam

EE221 - Practice for the Midterm Exam EE1 - Practice for the Midterm Exam 1. Consider this circuit and corresponding plot of the inductor current: Determine the values of L, R 1 and R : L = H, R 1 = Ω and R = Ω. Hint: Use the plot to determine

More information

EE5900 Spring Lecture 4 IC interconnect modeling methods Zhuo Feng

EE5900 Spring Lecture 4 IC interconnect modeling methods Zhuo Feng EE59 Spring Parallel LSI AD Algoriths Lecture I interconnect odeling ethods Zhuo Feng. Z. Feng MTU EE59 So far we ve considered only tie doain analyses We ll soon see that it is soeties preferable to odel

More information

BASIC PRINCIPLES. Power In Single-Phase AC Circuit

BASIC PRINCIPLES. Power In Single-Phase AC Circuit BASIC PRINCIPLES Power In Single-Phase AC Circuit Let instantaneous voltage be v(t)=v m cos(ωt+θ v ) Let instantaneous current be i(t)=i m cos(ωt+θ i ) The instantaneous p(t) delivered to the load is p(t)=v(t)i(t)=v

More information

B.E. / B.Tech. Degree Examination, April / May 2010 Sixth Semester. Electrical and Electronics Engineering. EE 1352 Power System Analysis

B.E. / B.Tech. Degree Examination, April / May 2010 Sixth Semester. Electrical and Electronics Engineering. EE 1352 Power System Analysis B.E. / B.Tech. Degree Examination, April / May 2010 Sixth Semester Electrical and Electronics Engineering EE 1352 Power System Analysis (Regulation 2008) Time: Three hours Answer all questions Part A (10

More information

Generators. What its all about

Generators. What its all about Generators What its all about How do we make a generator? Synchronous Operation Rotor Magnetic Field Stator Magnetic Field Forces and Magnetic Fields Force Between Fields Motoring Generators & motors are

More information

Lecture 11 - AC Power

Lecture 11 - AC Power - AC Power 11/17/2015 Reading: Chapter 11 1 Outline Instantaneous power Complex power Average (real) power Reactive power Apparent power Maximum power transfer Power factor correction 2 Power in AC Circuits

More information

Study Committee B5 Colloquium 2005 September Calgary, CANADA

Study Committee B5 Colloquium 2005 September Calgary, CANADA 36 Study oittee B olloquiu Septeber 4-6 algary, ND ero Sequence urrent opensation for Distance Protection applied to Series opensated Parallel Lines TKHRO KSE* PHL G BEUMONT Toshiba nternational (Europe

More information

Introduction to Synchronous. Machines. Kevin Gaughan

Introduction to Synchronous. Machines. Kevin Gaughan Introduction to Synchronous Machines Kevin Gaughan The Synchronous Machine An AC machine (generator or motor) with a stator winding (usually 3 phase) generating a rotating magnetic field and a rotor carrying

More information

Frame with 6 DOFs. v m. determining stiffness, k k = F / water tower deflected water tower dynamic response model

Frame with 6 DOFs. v m. determining stiffness, k k = F / water tower deflected water tower dynamic response model CE 533, Fall 2014 Undaped SDOF Oscillator 1 / 6 What is a Single Degree of Freedo Oscillator? The siplest representation of the dynaic response of a civil engineering structure is the single degree of

More information

2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL

2. A crack which is oblique (Swedish sned ) with respect to the xy coordinate system is to be analysed. TMHL (Del I, teori; 1 p.) 1. In fracture echanics, the concept of energy release rate is iportant. Fro the fundaental energy balance of a case with possible crack growth, one usually derives the equation where

More information

KINGS COLLEGE OF ENGINEERING Punalkulam

KINGS COLLEGE OF ENGINEERING Punalkulam KINGS COLLEGE OF ENGINEERING Punalkulam 613 303 DEPARTMENT OF ELECTRICAL AND ELECTRONICS ENGINEERING POWER SYSTEM ANALYSIS QUESTION BANK UNIT I THE POWER SYSTEM AN OVERVIEW AND MODELLING PART A (TWO MARK

More information

Exercise Dr.-Ing. Abdalkarim Awad. Informatik 7 Rechnernetze und Kommunikationssysteme

Exercise Dr.-Ing. Abdalkarim Awad. Informatik 7 Rechnernetze und Kommunikationssysteme Exercise1 1.10.015 Informatik 7 Rechnernetze und Kommunikationssysteme Review of Phasors Goal of phasor analysis is to simplify the analysis of constant frequency ac systems v(t) = max cos(wt + q v ) i(t)

More information

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) PH 1-A Fall 014 Waves - I Lectures 4-5 Chapter 16 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will

More information

EE 3120 Electric Energy Systems Study Guide for Prerequisite Test Wednesday, Jan 18, pm, Room TBA

EE 3120 Electric Energy Systems Study Guide for Prerequisite Test Wednesday, Jan 18, pm, Room TBA EE 3120 Electric Energy Systems Study Guide for Prerequisite Test Wednesday, Jan 18, 2006 6-7 pm, Room TBA First retrieve your EE2110 final and other course papers and notes! The test will be closed book

More information

THREE PHASE SYSTEMS Part 1

THREE PHASE SYSTEMS Part 1 ERT105: ELECTRCAL TECHNOLOGY CHAPTER 3 THREE PHASE SYSTEMS Part 1 1 Objectives Become familiar with the operation of a three phase generator and the magnitude and phase relationship. Be able to calculate

More information

Actuators & Mechanisms Actuator sizing

Actuators & Mechanisms Actuator sizing Course Code: MDP 454, Course Nae:, Second Seester 2014 Actuators & Mechaniss Actuator sizing Contents - Modelling of Mechanical Syste - Mechaniss and Drives The study of Mechatronics systes can be divided

More information

11. AC Circuit Power Analysis

11. AC Circuit Power Analysis . AC Circuit Power Analysis Often an integral part of circuit analysis is the determination of either power delivered or power absorbed (or both). In this chapter First, we begin by considering instantaneous

More information

Chapter 2: Introduction to Damping in Free and Forced Vibrations

Chapter 2: Introduction to Damping in Free and Forced Vibrations Chapter 2: Introduction to Daping in Free and Forced Vibrations This chapter ainly deals with the effect of daping in two conditions like free and forced excitation of echanical systes. Daping plays an

More information

Electric Power System Transient Stability Analysis Methods

Electric Power System Transient Stability Analysis Methods 1 Electric Power Syste Transient Stability Analysis Methods João Pedro de Carvalho Mateus, IST Abstract In this paper are presented the state of the art of Electric Power Syste transient stability analysis

More information

Modeling & Analysis of the International Space Station

Modeling & Analysis of the International Space Station Modeling & Analysis of the International Space Station 1 Physical Syste Solar Alpha Rotary Joints Physical Syste Rotor Stator Gear Train Solar Array Inboard Body Outboard Body +x Solar Array 3 Physical

More information

Sinusoidal Steady State Power Calculations

Sinusoidal Steady State Power Calculations 10 Sinusoidal Steady State Power Calculations Assessment Problems AP 10.1 [a] V = 100/ 45 V, Therefore I = 20/15 A P = 1 (100)(20)cos[ 45 (15)] = 500W, 2 A B Q = 1000sin 60 = 866.03 VAR, B A [b] V = 100/

More information

In this chapter we will start the discussion on wave phenomena. We will study the following topics:

In this chapter we will start the discussion on wave phenomena. We will study the following topics: Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical

More information

LONGER TERM STABILISATION OF WIND POWER PLANT VOLTAGE/REACTIVE POWER FLUCTUATIONS BY FACTS SOLUTION

LONGER TERM STABILISATION OF WIND POWER PLANT VOLTAGE/REACTIVE POWER FLUCTUATIONS BY FACTS SOLUTION LONGER TERM TABILIATION OF WIND POWER PLANT VOLTAGE/REACTIVE POWER FLUCTUATION BY FACT OLUTION NIJAZ DIZDAREVIĆ, MATILAV MAJTROVIĆ Energy Institute HRVOJE POŽAR avska 63, HR- Zagreb Croatia www.eihp.hr/~ndizdar

More information

Impedance seen by Distance Relays on Lines Fed from Fixed Speed Wind Turbines

Impedance seen by Distance Relays on Lines Fed from Fixed Speed Wind Turbines Ipedance seen by Distance Relays on Lines Fed fro Fixed Speed Wind Turbines Sachin Srivastava, Abhinna Chandra Biswal, Sethuraan Ganesan Power Technologies, ABB Corporate Research Bangalore sachin.srivastava@in.abb.co

More information

PROBLEM SOLUTIONS: Chapter 2

PROBLEM SOLUTIONS: Chapter 2 15 PROBLEM SOLUTIONS: Chapter 2 Problem 2.1 At 60 Hz, ω = 120π. primary: (V rms ) max = N 1 ωa c (B rms ) max = 2755 V, rms secondary: (V rms ) max = N 2 ωa c (B rms ) max = 172 V, rms At 50 Hz, ω = 100π.

More information

Week No. 6 Chapter Six: Power Factor Improvement

Week No. 6 Chapter Six: Power Factor Improvement Week No. 6 Chapter Six: Power Factor Improvement The electrical energy is almost wholly generated, transmitted and distributed in the form of alternating current. Therefore, the question of power factor

More information

EE2351 POWER SYSTEM ANALYSIS UNIT I: INTRODUCTION

EE2351 POWER SYSTEM ANALYSIS UNIT I: INTRODUCTION EE2351 POWER SYSTEM ANALYSIS UNIT I: INTRODUCTION PART: A 1. Define per unit value of an electrical quantity. Write equation for base impedance with respect to 3-phase system. 2. What is bus admittance

More information

Module 4. Single-phase AC Circuits

Module 4. Single-phase AC Circuits Module 4 Single-phase AC Circuits Lesson 14 Solution of Current in R-L-C Series Circuits In the last lesson, two points were described: 1. How to represent a sinusoidal (ac) quantity, i.e. voltage/current

More information

Sinusoidal Steady State Analysis (AC Analysis) Part II

Sinusoidal Steady State Analysis (AC Analysis) Part II Sinusoidal Steady State Analysis (AC Analysis) Part II Amin Electronics and Electrical Communications Engineering Department (EECE) Cairo University elc.n102.eng@gmail.com http://scholar.cu.edu.eg/refky/

More information

Consider Figure What is the horizontal axis grid increment?

Consider Figure What is the horizontal axis grid increment? Chapter Outline CHAPER 14 hree-phase Circuits and Power 14.1 What Is hree-phase? Why Is hree-phase Used? 14.2 hree-phase Circuits: Configurations, Conversions, Analysis 14.2.1 Delta Configuration Analysis

More information

SSC-JE EE POWER SYSTEMS: GENERATION, TRANSMISSION & DISTRIBUTION SSC-JE STAFF SELECTION COMMISSION ELECTRICAL ENGINEERING STUDY MATERIAL

SSC-JE EE POWER SYSTEMS: GENERATION, TRANSMISSION & DISTRIBUTION SSC-JE STAFF SELECTION COMMISSION ELECTRICAL ENGINEERING STUDY MATERIAL 1 SSC-JE STAFF SELECTION COMMISSION ELECTRICAL ENGINEERING STUDY MATERIAL Power Systems: Generation, Transmission and Distribution Power Systems: Generation, Transmission and Distribution Power Systems:

More information

Homework 2 SJTU233. Part A. Part B. Problem 2. Part A. Problem 1. Find the impedance Zab in the circuit seen in the figure. Suppose that R = 5 Ω.

Homework 2 SJTU233. Part A. Part B. Problem 2. Part A. Problem 1. Find the impedance Zab in the circuit seen in the figure. Suppose that R = 5 Ω. Homework 2 SJTU233 Problem 1 Find the impedance Zab in the circuit seen in the figure. Suppose that R = 5 Ω. Express Zab in polar form. Enter your answer using polar notation. Express argument in degrees.

More information

EKT103 ELECTRICAL ENGINEERING

EKT103 ELECTRICAL ENGINEERING EKT13 EECTRCA ENGNEERNG Chater 1 Three-Phase System 1 COURSE OUTCOME (CO) CO1: Ability to define and exlain the concet of single-hase and threehase system. 2 Revision A sinusoid is a signal that has the

More information

EE313 Fall 2013 Exam #1 (100 pts) Thursday, September 26, 2013 Name. 1) [6 pts] Convert the following time-domain circuit to the RMS Phasor Domain.

EE313 Fall 2013 Exam #1 (100 pts) Thursday, September 26, 2013 Name. 1) [6 pts] Convert the following time-domain circuit to the RMS Phasor Domain. Name If you have any questions ask them. Remember to include all units on your answers (V, A, etc). Clearly indicate your answers. All angles must be in the range 0 to +180 or 0 to 180 degrees. 1) [6 pts]

More information

BASIC NETWORK ANALYSIS

BASIC NETWORK ANALYSIS SECTION 1 BASIC NETWORK ANALYSIS A. Wayne Galli, Ph.D. Project Engineer Newport News Shipbuilding Series-Parallel dc Network Analysis......................... 1.1 Branch-Current Analysis of a dc Network......................

More information

University of Jordan Faculty of Engineering & Technology Electric Power Engineering Department

University of Jordan Faculty of Engineering & Technology Electric Power Engineering Department University of Jordan Faculty of Engineering & Technology Electric Power Engineering Department EE471: Electrical Machines-II Tutorial # 2: 3-ph Induction Motor/Generator Question #1 A 100 hp, 60-Hz, three-phase

More information

Force and dynamics with a spring, analytic approach

Force and dynamics with a spring, analytic approach Force and dynaics with a spring, analytic approach It ay strie you as strange that the first force we will discuss will be that of a spring. It is not one of the four Universal forces and we don t use

More information

PERIODIC STEADY STATE ANALYSIS, EFFECTIVE VALUE,

PERIODIC STEADY STATE ANALYSIS, EFFECTIVE VALUE, PERIODIC SEADY SAE ANALYSIS, EFFECIVE VALUE, DISORSION FACOR, POWER OF PERIODIC CURRENS t + Effective value of current (general definition) IRMS i () t dt Root Mean Square, in Czech boo denoted I he value

More information

IDAN Shock Mount Isolation Vibration Study November 1, The operation of shock and vibration isolation base plate

IDAN Shock Mount Isolation Vibration Study November 1, The operation of shock and vibration isolation base plate dr. Istvan Koller RTD USA BME Laboratory. Background In 998, Real Tie Devices USA, Inc. introduced a novel packaging concept for ebedded PC/04 odules to build Intelligent Data Acquisition Nodes. This syste,

More information

04-Electric Power. ECEGR 452 Renewable Energy Systems

04-Electric Power. ECEGR 452 Renewable Energy Systems 04-Electric Power ECEGR 452 Renewable Energy Systems Overview Review of Electric Circuits Phasor Representation Electrical Power Power Factor Dr. Louie 2 Introduction Majority of the electrical energy

More information

Chapter 10: Sinusoidal Steady-State Analysis

Chapter 10: Sinusoidal Steady-State Analysis Chapter 10: Sinusoidal Steady-State Analysis 1 Objectives : sinusoidal functions Impedance use phasors to determine the forced response of a circuit subjected to sinusoidal excitation Apply techniques

More information

POWER SYSTEM STABILITY

POWER SYSTEM STABILITY LESSON SUMMARY-1:- POWER SYSTEM STABILITY 1. Introduction 2. Classification of Power System Stability 3. Dynamic Equation of Synchronous Machine Power system stability involves the study of the dynamics

More information

Review of DC Electric Circuit. DC Electric Circuits Examples (source:

Review of DC Electric Circuit. DC Electric Circuits Examples (source: Review of DC Electric Circuit DC Electric Circuits Examples (source: http://hyperphysics.phyastr.gsu.edu/hbase/electric/dcex.html) 1 Review - DC Electric Circuit Multisim Circuit Simulation DC Circuit

More information

ELECTRIC POWER CIRCUITS BASIC CONCEPTS AND ANALYSIS

ELECTRIC POWER CIRCUITS BASIC CONCEPTS AND ANALYSIS Contents ELEC46 Power ystem Analysis Lecture ELECTRC POWER CRCUT BAC CONCEPT AND ANALY. Circuit analysis. Phasors. Power in single phase circuits 4. Three phase () circuits 5. Power in circuits 6. ingle

More information

LESSON 20 ALTERNATOR OPERATION OF SYNCHRONOUS MACHINES

LESSON 20 ALTERNATOR OPERATION OF SYNCHRONOUS MACHINES ET 332b Ac Motors, Generators and Power Systems LESSON 20 ALTERNATOR OPERATION OF SYNCHRONOUS MACHINES 1 LEARNING OBJECTIVES After this presentation you will be able to: Interpret alternator phasor diagrams

More information

ECE 421/521 Electric Energy Systems Power Systems Analysis I 2 Basic Principles. Instructor: Kai Sun Fall 2014

ECE 421/521 Electric Energy Systems Power Systems Analysis I 2 Basic Principles. Instructor: Kai Sun Fall 2014 ECE 41/51 Electric Energy Systems Power Systems Analysis I Basic Princiles Instructor: Kai Sun Fall 014 1 Outline Power in a 1-hase AC circuit Comlex ower Balanced 3-hase circuit Single Phase AC System

More information

Chapter 4. Synchronous Generators. Basic Topology

Chapter 4. Synchronous Generators. Basic Topology Basic Topology Chapter 4 ynchronous Generators In stator, a three-phase winding similar to the one described in chapter 4. ince the main voltage is induced in this winding, it is also called armature winding.

More information

Research on Capacitance Current Compensation Scheme of Current Differential Protection of Complex Four-Circuit Transmission Lines on the Same Tower

Research on Capacitance Current Compensation Scheme of Current Differential Protection of Complex Four-Circuit Transmission Lines on the Same Tower energies Article Research on apacitance urrent opensation Schee of urrent Differential Protection of oplex Four-ircuit Transission Lines on the Sae Tower ui Tang 1,2, * ID, Xianggen Yin 1,2 and Zhe Zhang

More information

Now multiply the left-hand-side by ω and the right-hand side by dδ/dt (recall ω= dδ/dt) to get:

Now multiply the left-hand-side by ω and the right-hand side by dδ/dt (recall ω= dδ/dt) to get: Equal Area Criterion.0 Developent of equal area criterion As in previous notes, all powers are in per-unit. I want to show you the equal area criterion a little differently than the book does it. Let s

More information

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous)

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad - 500 043 ELECTRICAL AND ELECTRONICS ENGINEERING QUESTION BANK Course Name : Computer Methods in Power Systems Course Code : A60222

More information

mywbut.com Lesson 16 Solution of Current in AC Parallel and Seriesparallel

mywbut.com Lesson 16 Solution of Current in AC Parallel and Seriesparallel esson 6 Solution of urrent in Parallel and Seriesparallel ircuits n the last lesson, the following points were described:. How to compute the total impedance/admittance in series/parallel circuits?. How

More information

Chapter 3 AUTOMATIC VOLTAGE CONTROL

Chapter 3 AUTOMATIC VOLTAGE CONTROL Chapter 3 AUTOMATIC VOLTAGE CONTROL . INTRODUCTION TO EXCITATION SYSTEM The basic function of an excitation system is to provide direct current to the field winding of the synchronous generator. The excitation

More information

a a a a a a a m a b a b

a a a a a a a m a b a b Algebra / Trig Final Exa Study Guide (Fall Seester) Moncada/Dunphy Inforation About the Final Exa The final exa is cuulative, covering Appendix A (A.1-A.5) and Chapter 1. All probles will be ultiple choice

More information

THREE-PHASE CIRCUITS. Historical Profiles

THREE-PHASE CIRCUITS. Historical Profiles C H A P T E R THREE-PHASE CIRCUITS 1 2 Society is never prepared to receive any invention. Every new thing is resisted, and it takes years for the inventor to get people to listen to him and years more

More information

In the previous chapter, attention was confined

In the previous chapter, attention was confined 4 4 Principles of Power System CHAPTE CHAPTE 8 Unsymmetrical Fault Calculations 8. Usymmetrical Faults on -Phase System 8. Symmetrical Components Method 8. Operator a 8.4 Symmetrical Components in Terms

More information

General Properties of Radiation Detectors Supplements

General Properties of Radiation Detectors Supplements Phys. 649: Nuclear Techniques Physics Departent Yarouk University Chapter 4: General Properties of Radiation Detectors Suppleents Dr. Nidal M. Ershaidat Overview Phys. 649: Nuclear Techniques Physics Departent

More information

Chapter 1: Basics of Vibrations for Simple Mechanical Systems

Chapter 1: Basics of Vibrations for Simple Mechanical Systems Chapter 1: Basics of Vibrations for Siple Mechanical Systes Introduction: The fundaentals of Sound and Vibrations are part of the broader field of echanics, with strong connections to classical echanics,

More information

Power Systems - Basic Concepts and Applications - Part I

Power Systems - Basic Concepts and Applications - Part I PDHonline Course E104 (1 PDH) Power ystems Basic Concepts and Applications Part I Instructor: hihmin Hsu PhD PE 01 PDH Online PDH Center 57 Meadow Estates Drive Fairfax A 006658 Phone & Fax: 709880088

More information

Power Factor Improvement

Power Factor Improvement Salman bin AbdulazizUniversity College of Engineering Electrical Engineering Department EE 2050Electrical Circuit Laboratory Power Factor Improvement Experiment # 4 Objectives: 1. To introduce the concept

More information

Chapter 8: Unsymmetrical Faults

Chapter 8: Unsymmetrical Faults Chapter 8: Unsymmetrical Faults Introduction The sequence circuits and the sequence networks developed in the previous chapter will now be used for finding out fault current during unsymmetrical faults.

More information

Electromagnetic fields modeling of power line communication (PLC)

Electromagnetic fields modeling of power line communication (PLC) Electroagnetic fields odeling of power line counication (PLC) Wei Weiqi UROP 3 School of Electrical and Electronic Engineering Nanyang echnological University E-ail: 4794486@ntu.edu.sg Keyword: power line

More information

Chapter 33. Alternating Current Circuits

Chapter 33. Alternating Current Circuits Chapter 33 Alternating Current Circuits 1 Capacitor Resistor + Q = C V = I R R I + + Inductance d I Vab = L dt AC power source The AC power source provides an alternative voltage, Notation - Lower case

More information

AC Power Analysis. Chapter Objectives:

AC Power Analysis. Chapter Objectives: AC Power Analysis Chapter Objectives: Know the difference between instantaneous power and average power Learn the AC version of maximum power transfer theorem Learn about the concepts of effective or value

More information

PHYS 102 Previous Exam Problems

PHYS 102 Previous Exam Problems PHYS 102 Previous Exa Probles CHAPTER 16 Waves Transverse waves on a string Power Interference of waves Standing waves Resonance on a string 1. The displaceent of a string carrying a traveling sinusoidal

More information

Chapter 5 Steady-State Sinusoidal Analysis

Chapter 5 Steady-State Sinusoidal Analysis Chapter 5 Steady-State Sinusoidal Analysis Chapter 5 Steady-State Sinusoidal Analysis 1. Identify the frequency, angular frequency, peak value, rms value, and phase of a sinusoidal signal. 2. Solve steady-state

More information

The Operation of a Generator on Infinite Busbars

The Operation of a Generator on Infinite Busbars The Operation of a Generator on Infinite Busbars In order to simplify the ideas as much as possible the resistance of the generator will be neglected; in practice this assumption is usually reasonable.

More information

A Simplified Analytical Approach for Efficiency Evaluation of the Weaving Machines with Automatic Filling Repair

A Simplified Analytical Approach for Efficiency Evaluation of the Weaving Machines with Automatic Filling Repair Proceedings of the 6th SEAS International Conference on Siulation, Modelling and Optiization, Lisbon, Portugal, Septeber -4, 006 0 A Siplified Analytical Approach for Efficiency Evaluation of the eaving

More information

Lecture #8-3 Oscillations, Simple Harmonic Motion

Lecture #8-3 Oscillations, Simple Harmonic Motion Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.

More information

EE 6501 POWER SYSTEMS UNIT I INTRODUCTION

EE 6501 POWER SYSTEMS UNIT I INTRODUCTION EE 6501 POWER SYSTEMS UNIT I INTRODUCTION PART A (2 MARKS) 1. What is single line diagram? A Single line diagram is diagrammatic representation of power system in which the components are represented by

More information

Fourier Series Summary (From Salivahanan et al, 2002)

Fourier Series Summary (From Salivahanan et al, 2002) Fourier Series Suary (Fro Salivahanan et al, ) A periodic continuous signal f(t), - < t

More information

Exam 3 Solutions. 1. Which of the following statements is true about the LR circuit shown?

Exam 3 Solutions. 1. Which of the following statements is true about the LR circuit shown? PHY49 Spring 5 Prof. Darin Acosta Prof. Paul Avery April 4, 5 PHY49, Spring 5 Exa Solutions. Which of the following stateents is true about the LR circuit shown? It is (): () Just after the switch is closed

More information

Mutual capacitor and its applications

Mutual capacitor and its applications Mutual capacitor and its applications Chun Li, Jason Li, Jieing Li CALSON Technologies, Toronto, Canada E-ail: calandli@yahoo.ca Published in The Journal of Engineering; Received on 27th October 2013;

More information

QUESTION BANK ENGINEERS ACADEMY. Power Systems Power System Stability 1

QUESTION BANK ENGINEERS ACADEMY. Power Systems Power System Stability 1 ower ystems ower ystem tability QUETION BANK. A cylindrical rotor generator delivers 0.5 pu power in the steady-state to an infinite bus through a transmission line of reactance 0.5 pu. The generator no-load

More information

= 32.0\cis{38.7} = j Ω. Zab = Homework 2 SJTU233. Part A. Part B. Problem 2. Part A. Problem 1

= 32.0\cis{38.7} = j Ω. Zab = Homework 2 SJTU233. Part A. Part B. Problem 2. Part A. Problem 1 Homework 2 SJTU233 Problem 1 Find the impedance Zab in the circuit seen in the figure. Suppose that R = 5 Ω. Express Zab in polar form. Enter your answer using polar notation. Express argument in degrees.

More information

Review of Basic Electrical and Magnetic Circuit Concepts EE

Review of Basic Electrical and Magnetic Circuit Concepts EE Review of Basic Electrical and Magnetic Circuit Concepts EE 442-642 Sinusoidal Linear Circuits: Instantaneous voltage, current and power, rms values Average (real) power, reactive power, apparent power,

More information

Revised October 6, EEL , Henry Zmuda. 2. Three-Phase Circuits 1

Revised October 6, EEL , Henry Zmuda. 2. Three-Phase Circuits 1 Three Phase Circuitsit Revised October 6, 008. Three-Phase Circuits 1 Preliminary Comments and a quick review of phasors. We live in the time domain. We also assume a causal (nonpredictive) world. Real-world

More information

Physics 2107 Oscillations using Springs Experiment 2

Physics 2107 Oscillations using Springs Experiment 2 PY07 Oscillations using Springs Experient Physics 07 Oscillations using Springs Experient Prelab Read the following bacground/setup and ensure you are failiar with the concepts and theory required for

More information

Sinusoidal Response of RLC Circuits

Sinusoidal Response of RLC Circuits Sinusoidal Response of RLC Circuits Series RL circuit Series RC circuit Series RLC circuit Parallel RL circuit Parallel RC circuit R-L Series Circuit R-L Series Circuit R-L Series Circuit Instantaneous

More information

Dr. Naser Abu-Zaid; Lecture notes in electromagnetic theory 1; Referenced to Engineering electromagnetics by Hayt, 8 th edition 2012; Text Book

Dr. Naser Abu-Zaid; Lecture notes in electromagnetic theory 1; Referenced to Engineering electromagnetics by Hayt, 8 th edition 2012; Text Book Text Book Dr. Naser Abu-Zaid Page 1 9/4/2012 Course syllabus Electroagnetic 2 (63374) Seester Language Copulsory / Elective Prerequisites Course Contents Course Objectives Learning Outcoes and Copetences

More information

12. Introduction and Chapter Objectives

12. Introduction and Chapter Objectives Real Analog - Circuits 1 Chapter 1: Steady-State Sinusoidal Power 1. Introduction and Chapter Objectives In this chapter we will address the issue of power transmission via sinusoidal or AC) signals. This

More information

Module 4. Single-phase AC circuits. Version 2 EE IIT, Kharagpur

Module 4. Single-phase AC circuits. Version 2 EE IIT, Kharagpur Module 4 Single-phase circuits ersion EE T, Kharagpur esson 6 Solution of urrent in Parallel and Seriesparallel ircuits ersion EE T, Kharagpur n the last lesson, the following points were described:. How

More information

Successful Brushless A.C. Power Extraction From The Faraday Acyclic Generator

Successful Brushless A.C. Power Extraction From The Faraday Acyclic Generator Successful Brushless A.C. Power Extraction Fro The Faraday Acyclic Generator July 11, 21 Volt =.2551552 volt 1) If we now consider that the voltage is capable of producing current if the ri of the disk

More information

Brief Steady of Power Factor Improvement

Brief Steady of Power Factor Improvement International Journal of Electrical Engineering. ISSN 0974-2158 Volume 6, Number 5 (2013), pp. 531-539 International Research PublicationHouse http://www.irphouse.com Brief Steady of Power Factor Improvement

More information