power system fundamentals ee-317 lecture 3 06 october 2010

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Power System Power System Fundamentals Fundamentals EE-317 EE-317 Lecture 3 Lecture 3 06 October 2010

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Page 1: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Power System Power System FundamentalsFundamentalsPower System Power System FundamentalsFundamentals

EE-317EE-317Lecture 3Lecture 3

06 October 2010

Page 2: Power System Fundamentals EE-317 Lecture 3 06 October 2010

AimsAims

Finish Chapter 1 – Real and Reactive PowerReal and Reactive LoadsPower Triangle

Chapter 2 – Three Phase Circuits Chapter 3 – Transformers

Page 3: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Sine Wave Basics (Review)Sine Wave Basics (Review) RMS – a method for computing the effective value of a time-varying e-m

wave, equivalent to the energy under the area of the voltage waveform.

Page 4: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Real, Reactive and Apparent Power in AC Circuits

Real, Reactive and Apparent Power in AC Circuits in DC circuits: P=VI but…= in AC circuits: average power

supplied to the load will be affected by the phase angle between the voltage and the current.

If load is inductive the phase angle (also called impedance angle) is positive; (i.e, phase angle of current will lag the phase angle of the voltage) and the load will consume both real and positive reactive power

If the load is capacitive the impedance angle will be negative (the phase angle of the current will lead the phase angle of the voltage) and the load will consume real power and supply reactive power.

Page 5: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Resistive and Reactive LoadsResistive and Reactive Loads

Page 6: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Impedance Angle, Current Angle & PowerImpedance Angle, Current Angle & Power Inductive loads positive impedance angle

current angle lags voltage angle Capacitive loads negative impedance angle

current angle leads voltage angle

Both types of loads consume real power One (inductive) consumes reactive as well while

the other (capacitive) supplies reactive power

Page 7: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Useful EquationsUseful Equations

First term is average or Real power (P) Second term is power transferred back and forth

between source and load (Reactive power- Q)

Page 8: Power System Fundamentals EE-317 Lecture 3 06 October 2010

More equationsMore equations

Real term averages to P = VI cos (+) Reactive term averages to Q = VI sin (+/-)

Reactive power is the power that is first stored and then released

in the magnetic field of an inductor or in the electric field of a capacitor

Apparent Power (S) is just = VI

Page 9: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Loads with Constant ImpedanceLoads with Constant Impedance V = IZ

Substituting… P = I2Z cos Q = I2Z sin S= I2Z

Since… Z = R + jX = Z cos + jZ sin P = I2R and Q = I2X

Page 10: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Complex Power and Key Relationship of Phase Angle to V&I

Complex Power and Key Relationship of Phase Angle to V&I

S = P + jQ S = VI(complex conjugate operator) If V = V30o and I = I15o

THEN….. COMPLEX POWER SUPPLIED TO LOAD = S = (V30o)(I-15o) = VI (30o-15o )= VI cos(15o ) + jVI sin(15o )

NOTE: Since Phase Angle = V - IS = VI cos() + jVI sin() = P + jQ

Page 11: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Review V, I, ZReview V, I, Z

If load is inductive then the Phase Angle (Impedance Angle Z) is positive, If phase angle is positive, the phase angle of the current flowing through the load will lag the voltage phase angle across the load by the impedance angle Z.

Page 12: Power System Fundamentals EE-317 Lecture 3 06 October 2010

The Power TriangleThe Power Triangle

Page 13: Power System Fundamentals EE-317 Lecture 3 06 October 2010

ExampleExample

V = 2400o V Z = 40-30o

Calculate current I, Power Factor (is it leading or lagging), real, reactive, apparent and complex power supplied to the load

Page 14: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Read Chapters 2 & 3Read Chapters 2 & 3

HW Assignment 2: Problems 1-9, 1-15, 1-18, 1-19, 2-4

Page 15: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Example ProblemExample Problem

HW 1-19 (a)

Page 16: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Chapter 2Chapter 2

Three-Phase (3-) CircuitsWhat are they? Benefits of 3- SystemsGenerating 3- Voltages and CurrentsWye (Y) and delta () connectionsBalanced systemsOne-Line Diagrams

Page 17: Power System Fundamentals EE-317 Lecture 3 06 October 2010

What does Three-Phase mean?What does Three-Phase mean?

A 3- circuit is a 3- AC-generation system serving a 3- AC load

3 - 1- AC generators with equal voltage but phase angle differing from the others by 120o

Page 18: Power System Fundamentals EE-317 Lecture 3 06 October 2010
Page 19: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Multiple poles….Multiple poles….

Page 20: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Benefits of 3- circuitsBenefits of 3- circuits

GENERATION SIDE: More power per kilogram Constant power out (vs. pulsating sinusoidal)

LOAD SIDE: Induction Motors (no starters required)

Page 21: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Common NeutralCommon Neutral

A 3- circuit can have the negative ends of the 3- generators connected to the negative ends of the 3- AC loads and one common neutral wire can complete the system

If the three loads are equal (or balanced) what will the return current be in the common neutral?

Page 22: Power System Fundamentals EE-317 Lecture 3 06 October 2010

If loads are equal….If loads are equal….

the return current can be calculated to be… ZERO! (see trig on p. 59 for more detail) Neutral is actually unnecessary in a balanced

three-phase system (but is provided since circumstances may change)

Page 23: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Wye (Y) and delta () connectionWye (Y) and delta () connection

Page 24: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Delta () Delta ()

Page 25: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Y and Y and

Y-connectionIL = IVLL = 3 V

-connectionVLL = V

IL = 3 I

Page 26: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Balanced systemsBalanced systems

Page 27: Power System Fundamentals EE-317 Lecture 3 06 October 2010

One-Line DiagramsOne-Line Diagrams

since all phases are same (except for phase angle) and loads are typically balanced only one of the phases is usually shown on an electrical diagram… it is called a one-line diagram

Typically include all major components of the system (generators, transformers, transmission lines, loads, other [regulators, swithes])

Page 28: Power System Fundamentals EE-317 Lecture 3 06 October 2010

Chapter 3Chapter 3

TransformersBenefits of TransformersTypes and Construction, The Ideal TransformerTransformer Efficiency and Voltage RegulationTransformer TapsAutotransformers3- Transformer connections– Y-Y, Y-, -Y, -

Page 29: Power System Fundamentals EE-317 Lecture 3 06 October 2010

BenefitsBenefits

Range of Power Systems Power Levels Seamless Converter of Power (Voltage) Reduced Transmission Losses Efficient Converter Low Maintenance (min. moving parts) Enables Utilization of Power at nearly all levels