chapter 14 – basic elements and phasors lecture 17 by moeen ghiyas 13/12/2015 1

36
Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 12/06/22 1

Upload: vincent-reeves

Post on 17-Jan-2016

225 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Chapter 14 – Basic Elements and Phasors

Lecture 17

by Moeen Ghiyas

21/04/23 1

Page 2: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Chapter 14 – Basic Elements and Phasors

Page 3: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Average Power & Power Factor

Complex Numbers

Math Operations with Complex Numbers

Page 4: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

We know for any load

v = Vm sin(ωt + θv)

i = Im sin(ωt + θi)

Then the power is defined by

Using the trigonometric identity

Thus, sine function becomes

Page 5: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Putting above values in

We have

The average value of 2nd term is zero over one cycle, producing

no net transfer of energy in any one direction.

The first term is constant (not time dependent) is referred to as

the average power or power delivered or dissipated by the load.

Page 6: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1
Page 7: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Since cos(–α) = cos α,

the magnitude of average power delivered is independent of whether v

leads i or i leads v.

Ths, defining θ as equal to | θv – θi |, where | | indicates that only the

magnitude is important and the sign is immaterial, we have average

power or power delivered or dissipated as

Page 8: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

The above eq for average power can also be written as

But we know Vrms and Irms values as

Thus average power in terms of vrms and irms becomes,

21/04/23 8

Page 9: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

For resistive load,

We know v and i are in phase, then |θv - θi| = θ = 0°,

And cos 0° = 1, so that

becomes

or

Page 10: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

For inductive load ( or network),

We know v leads i, then |θv - θi| = θ = 90°,

And cos 90° = 0, so that

Becomes

Thus, the average power or power dissipated by the ideal

inductor (no associated resistance) is zero watts.

Page 11: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

For capacitive load ( or network),

We know v lags i, then |θv - θi| = |–θ| = 90°,

And cos 90° = 0, so that

Becomes

Thus, the average power or power dissipated by the ideal

capacitor is also zero watts.

Page 12: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Power Factor

In the equation,

the factor that has significant control over the delivered power

level is cos θ.

No matter how large the voltage or current, if cos θ = 0, the

power is zero; if cos θ = 1, the power delivered is a maximum.

Since it has such control, the expression was given the name

power factor and is defined by

For situations where the load is a combination of resistive and

reactive elements, the power factor will vary between 0 and 1

Page 13: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

In terms of the average power, we know power factor is

The terms leading and lagging are often written in conjunction

with power factor and defined by the current through load.

If the current leads voltage across a load, the load has a leading

power factor. If the current lags voltage across the load, the load

has a lagging power factor.

In other words, capacitive networks have leading power factors,

and inductive networks have lagging power factors.

Page 14: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Determine the average power delivered to network

having the following input voltage and current:

v = 150 sin(ωt – 70°) and i = 3 sin(ωt – 50°)

Solution

Page 15: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Determine the power factors of the following loads,

and indicate whether they are leading or lagging:

Solution:

Page 16: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Determine the power factors of the following loads,

and indicate whether they are leading or lagging:

Solution:

Page 17: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Application of complex numbers result in a technique for finding

the algebraic sum of sinusoidal waveforms

A complex number represents a point in a two-dimensional

plane located with reference to two distinct axes.

The horizontal axis is called the real axis, while the vertical axis

is called the imaginary axis.

The symbol j (or sometimes i) is

used to denote the imaginary

component.

Page 18: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Two forms are used to represent a

complex number:

rectangular and polar.

Rectangular Form

Polar Form

Page 19: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Polar Form

θ is always measured counter-clockwise

(CCW) from the positive real axis.

Angles measured in the clockwise direction

from the positive real axis must have a

negative sign

Page 20: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Sketch the following complex numbers in the

complex plane:

a. C = 3 + j 4 b. C = 0 - j 6

Page 21: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Sketch the following complex numbers in the

complex plane:

c. C = -10 - j20

Page 22: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Sketch the following complex numbers in the

complex plane:

Page 23: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Sketch the following complex numbers in the

complex plane:

Page 24: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Rectangular to Polar

Polar to Rectangular

Angle determined to be

associated carefully with the

magnitude of the vector as per

the quadrant in which complex

number lies

Page 25: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Convert the following from polar to rectangular form:

Solution:

Page 26: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Convert the following from rectangular to polar form:

C = - 6 + j 3

Solution:

Page 27: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

EXAMPLE - Convert the following from polar to rectangular form:

Solution

Page 28: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Let us first examine the symbol j associated with imaginary

numbers. By definition,

Page 29: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

The conjugate or complex conjugate is found

by changing sign of imaginary part in rectangular form

or by using the negative of the angle of the polar form.

Rectangular form,

Polar form,

(conjugate)

(conjugate)

Page 30: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Addition Example (Rectangular)

Add C1 = 3 + j 6 and C2 = -6 + j 3.

Solution

Page 31: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Subtraction Example (Rectangular)

Solution

Page 32: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Imp Note

Addition or subtraction cannot be performed in polar

form unless the complex numbers have the same

angle θ or unless they differ only by multiples of 180°.

Page 33: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Addition Example (Polar)

Page 34: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Subtraction Example (Polar)

Page 35: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

Average Power & Power Factor

Complex Numbers

Math Operations with Complex Numbers

Page 36: Chapter 14 – Basic Elements and Phasors Lecture 17 by Moeen Ghiyas 13/12/2015 1

21/04/23 36