45
CHAPTER 4 : FOURIER SERIES 4.0 Introduction A periodic signal x(t) is periodic if x(t + T) = x (t) where T is the period and . Sinusoid of frequency nf 0 where n is positive integer is said to be the n th harmonic. If: n = odd (odd harmonic) n = even (even harmonic) 4.1 Trigonometric Fourier series If x(t) is a periodic function with period T, then x(t) can be expressed as trigonometric Fourier series: x(t) is expressed as the sum of sinusoidal components having different frequencies where: and - the Fourier coefficients - the dc value of x(t) 4.1.1 Orthogonal Fuctions for Sine and Cosine Functions Consider a function and . According to orthogonal function properties Where m and n are integers, T is the period and r n is some value. Let and , then

Chapter 4-Fourier Series

Embed Size (px)

Citation preview

Page 1: Chapter 4-Fourier Series

CHAPTER 4 : FOURIER SERIES

4.0 Introduction

A periodic signal x(t) is periodic if x(t + T) = x (t) where T is the period and .

Sinusoid of frequency nf0 where n is positive integer is said to be the nth harmonic. If:

n = odd (odd harmonic)

n = even (even harmonic)

4.1 Trigonometric Fourier series

If x(t) is a periodic function with period T, then x(t) can be expressed as trigonometric

Fourier series:

x(t) is expressed as the sum of sinusoidal components having different frequencies

where:

and - the Fourier coefficients

- the dc value of x(t)

4.1.1 Orthogonal Fuctions for Sine and Cosine Functions

Consider a function and . According to orthogonal function properties

Where m and n are integers, T is the period and rn is some value.

Let and , then

1)

If n = 0, then

2)

Let and , then

3)

Page 2: Chapter 4-Fourier Series

Let and , then

4)

If n = 0, then

5)

4.1.2 Determination of Trigonometric Fourier Coefficients

4.1.2.1 Determination of Fourier coefficient, :

Based on the trigonometric Fourier series expression

(4.1.2)

When Equation (4.1.2) is integrated both sides for one complete cycle, then

Using Orthogonal functions relation.

Thus,

4.1.2.2 Determination of Fourier coefficient, :

When Equation (4.1.2) is multiplied both sides with and then

integrated for one complete cycle, then

Page 3: Chapter 4-Fourier Series

Using orthogonal function relation,

and

then,

Since m = n, then

4.1.2.3 Determination of Fourier coefficient, :

When Equation (4.1.2) is multiplied both sides with and then

integrated for one complete cycle, then

Using Orthogonal functions relation,

And

Page 4: Chapter 4-Fourier Series

then,

Since m = n, then

Graph of sin nωt

Sin 2nπ n = even 0 0

Page 5: Chapter 4-Fourier Series

n = odd 0Sin nπ n = even 0 0

n = odd 0

Sin

n = even 0 0n = odd 1,-1, 1,-1, 1

n = both 1, 0,-1, 1, 0,

where n = 2n-1

Graph of cos nωt

Cos 2nπ n = even 1 1n = odd 1

Cos nπ n = even 1n = odd -1

Cos

n = even -1, 1, -1, 1,

n = odd 0 0n = both 0,-1, 0, 1, 0, Cos(2n - 1)π = -1

where n = 2n-1

Example 4.1.1 Express the signal x(t) shown in Figure 4.1.1 as trigonometric

Fourier series.

Figure 4.1.1

SOLUTION:

Page 6: Chapter 4-Fourier Series

The average value, is determined as follows:

or

= [Area under the curve for one complete cycle]

The Fourier coefficient, is determined as follows:

Page 7: Chapter 4-Fourier Series

Since: sin nπ = 0 and sin 2nπ = 0;

The Fourier coefficient, bn is determined as follows:

Since: cos nπ = (-1)n and cos 2nπ = 1;

Thus,

or

Example 4.1.2 Express signal the x(t) shown in Figure 4.1.2 as trigonometric Fourier

series

Page 8: Chapter 4-Fourier Series

Figure 4.1.2

SOLUTION:

The average value, is determined as follows:

or

= [Area under the curve for one complete cycle]

The Fourier coefficient, is determined as follows:

Page 9: Chapter 4-Fourier Series

Since: sin nπ = 0 and sin 2nπ = 0;

The Fourier coefficient, bn is determined as follows:

Page 10: Chapter 4-Fourier Series

Thus,

4.2 Symmetry Properties

i) Even Symmetry

ii) Odd Symmetry

iii) Half-Wave Symmetry

iv) Even And Half-Wave Symmetry (Half-Wave Even Symmetry)

v) Odd And Half-Wave Symmetry (Half-Wave Odd Symmetry)

vi) Hidden symmetry

Page 11: Chapter 4-Fourier Series

4.2.1 Even Symmetry

Example 4.2.1 Consider a half-cycle signal x(t) shown in Figure 4.2.1(a) where T = 2

sec.

Figure 4.2.1(a)

The signal x(t) is said to be even symmetry if x(t) = x(-t). This-property is shown in

Figure 4.2.1(b)

Figure 4.2.1(b)

The even-symmetry signal x(t) for 3 complete cycles is shown in Figure 4.2.1(c).

Page 12: Chapter 4-Fourier Series

Figure 4.2.1(c)

4.2.2 Odd Symmetry

Example 4.2.2 Consider a half-cycle signal x(t) shown in Figure 4.2.2(a) where T = 2

sec.

Figure 4.2.2(a)

The signal x(t) is said to be odd symmetry if x(t) = -x(-t). This property is shown in

Figure 4.2.2(b)

Figure 4.2.2(b)

1 cycle 1 cycle 1 cycle

Page 13: Chapter 4-Fourier Series

The odd-symmetry signal x(t) for 3 complete cycles is shown in Figure 4.2.2(c)

Figure 4.2.2(c)

4.2.3 Half-Wave Symmetry

Example 4.2.3 Consider a half-cycle signal x(t) shown in Figure 4.2.3(a) where T = 2

sec.

Figure 4.2.3(a)

The signal x(t) is said to be half-wave symmetry if x(t) = -x(t + T/2). This property is

shown in Figure 4.2.3(b)

1 cycle 1 cycle 1 cycle

Page 14: Chapter 4-Fourier Series

Figure 4.2.3(b)

The half-wave symmetry signal x(t) for 3 complete cycles is shown in Figure 4.2.3(c).

Figure 4.2.3(c)

4.2.4 Even and Half-Wave Symmetry (Half-Wave Even Symmetry)

Example 4.2.4 Consider a half-cycle signal x(t) shown in Figure 4.2.4(a) where T =

4 sec.

Figure 4.2.4(a)

For one complete cycle/the shape of signal x(t) is the same for both properties. This is

shown in Figure 4.2.4(b).

1 cycle 1 cycle 1 cycle

Page 15: Chapter 4-Fourier Series

Figure 4.2.4(b)

Thus, the half-wave even symmetry signal x(t) for 3 complete cycles is shown in Figure

4.2.4(c).

Figure 4.2.4(c)

4.2.4 Odd and Half-Wave Symmetry (Half-Wave Odd Symmetry)

Example 4.2.5 Consider a half-cycle signal x(t) shown in Figure 4.2.5(a) where T

= 4 sec.

Figure 4.2.5(a)

1 cycle 1 cycle 1 cycle

Page 16: Chapter 4-Fourier Series

For one complete cycle, the shape of signal x(t) is the same for both properties.This is

shown in Figure 4.2.5(b).

Figure 4.2.5(b)

Thus, the half-wave even symmetry signal x(t) for 3 complete cycles is shown in Figure

4.2.5 (c).

Figure 4.2.5 (c)

Example 4.2.6 The first half-cycle of a periodic signal y(t) is shown in Figure

4.2.6(a) and the period sec. Sketch y(t) clearly for.3

complete cycles if:

i) y(t) is an even-symmetric signal

ii) y(t) is an odd-symmetric signal

iii) y(t) is a half-wave symmetric signal

1 cycle 1 cycle 1 cycle

Page 17: Chapter 4-Fourier Series

Figure 4.2.6(a)

SOLUTION:

The signal y(t) for all cases are given in Figure 4.2.6(b).

Page 18: Chapter 4-Fourier Series

Figure 4.2.6(b)

4.3 Effects of Symmetry

i) If x(t) is an even symmetric signal, then its trigonometric Fourier series

expression is as follows:

Its Fourier series consists of a constant and cosine terms only where:

ii) If x(t) is an odd symmetric signal, then its trigonometric Fourier series

expression is as follows:

Its Fourier series consists of sine terms only where:

and

iii) If x(t) is a half-wave symmetric signal, then its trigonometric Fourier expression

is as follows:

Its Fourier series consists of odd harmonic of cosine and sine terms only where:

, and

Page 19: Chapter 4-Fourier Series

iv) If x(t) is an even symmetric and also half-wave symmetric signal (half-wave

even symmetric signal), then its trigonometric Fourier series expression is as

follows:

Its Fourier series consists of a constant and cosine terms only where:

, and

v) If x(t) is an odd symmetric and also half-wave symmetric signal (half-wave odd

symmetric), then its trigonometric Fourier series expression is as follows:

Its Fourier series consists of odd harmonic of sine terms only where:

, and

Page 20: Chapter 4-Fourier Series

The trigonometric Fourier series expressions of each symmetric signal are summarized

in Table 4.1.

Table 4.1 Fourier series Simplified Flow Techniques

Signal function

TFS Coefficients

Coefficients TFS expressions

Generala0

an

bn

Even symmetry

a0

an

bn=0

Odd symmetry

bn

a0 = an = 0

Half-wave symmetry

a0 =0

an (even) =0

bn (even) =0

Even and half-wave symmetry

a0 =0

bn =0

an (even) =0

Odd and half-wave symmetry

a0 =0

an =0

bn (even) =0

Page 21: Chapter 4-Fourier Series

Example 4.3.1 Express signal x(t) shown in Figure 4.3.1 as trigonometric Fourier

series using symmetry property.

Figure 4.3.1

SOLUTION:

The signal x(t) is odd-symmetry and half- wave symmetry signal (half-wave odd

symmetry).

, and

The Fourier coefficient is determined as follows:

Page 22: Chapter 4-Fourier Series

Thus,

Example 4.3.2 Express signal x(t) shown in Figure 4.3.2 as trigonometric Fourier

series using Symmetry property.

Figure 4.3.2

SOLUTION:

x(t) is even-symmetry and half- wave symmetry signal (half-wave even symmetry).

, and

The Fourier coefficient is determined as follows:

Page 23: Chapter 4-Fourier Series

Thus,

4.4 Hidden Symmetry

Example 4.4.1 Express signal x(t) as trigonometric Fourier series.

Page 24: Chapter 4-Fourier Series

Figure 4.4.1(a)

SOLUTION:

Signal x(t) does not posses any symmetry properties. The evaluation can be further

simplified by shifting the dc value of signal x(t). Signal g(t) is obtain from signal x(t)

where x(t) = 0.5A + g(t) and signal g(t) is shown in Figure 4.4.1 (b).

Figure 4.4.1 (b)

Signal g(t) posses odd-symmetry property. Thus,

Fourier series of x(t) = 0.5A + Fourier series of g(t)

For odd Symmetric signal, then

and

The Fourier coefficient, bn is determined as follows:

Page 25: Chapter 4-Fourier Series
Page 26: Chapter 4-Fourier Series

Thus,

Fourier series of x(t) = 0.5A + Fourier series of g(t)

Example 4.4.2 Express the signal x (t) shown in Figure 4.4.2(a) as trigonometric

Fourier series.

Figure 4.4.2(a)

SOLUTION:

Signal x(t) posses even-symmetry property. The evaluation can be further simplified by

shifting the dc value of signal x(t). Signal g(t) is obtain from signal x(t) where signal

and the signal g(t) is shown in Figure 4.4.2(b).

Figure 4.4.2(b)

Signal g(t) posses half-wave even symmetry property. Thus,

Page 27: Chapter 4-Fourier Series

Fourier series of x(t) = + Fourier series of g(t)

Fourier series of g(t) is obtain as follows:

, and

The Fourier coefficient, an (n=odd) is determined as follows:

Page 28: Chapter 4-Fourier Series

Fourier series of x(t) = + Fourier series of g(t)

Page 29: Chapter 4-Fourier Series

4.5 Exponential Fourier series

The trigonometric Fourier series of signal x(t) is given as:

EULER'S IDENTITY:

The expression can be expressed as follows:

Let , and

Then,

The term can also be represented as follows:

Then,

Where:

Page 30: Chapter 4-Fourier Series

EULER'S IDENTITY:

Then, where n = ±1, ±2, ….

Example 4.5.1 Express the signal x(t) shown in Figure 4.5.1 as an exponential

Fourier series.

Figure 4.5.1

SOLUTION:

Page 31: Chapter 4-Fourier Series

EULER IDENTITY:

Then,

and

Thus,

Example 4.5.2 Express the signal x (t) shown in Figure 4.5.2 as an exponential

Fourier series.

Page 32: Chapter 4-Fourier Series

Figure 4.5.2

SOLUTION:

EULER IDENTITY:

Page 33: Chapter 4-Fourier Series

Then,

For n = 0, Cn has no meaning. Thus,

Thus,

4.6 Frequency Spectrum

Frequency spectrum consists of amplitude and phase spectrums. Amplitude spectrum

is the plot of |Cn| versus and phase spectrum is the plot of versus .

ASIDE:

To determine the amplitude and phase spectrums of Frequency spectrum, the

magnitude and phase of X are shown in Figure 4.6 and summarized in Table 4.6:

Page 34: Chapter 4-Fourier Series

Figure 4.6

Table 4.6

Magnitude Amplitude

spectrums

Phase spectrums

1 X = a + jb |X| =

2 X = jb |X| = b

3 X = -jb |X| = b

4 X = a |X| = a

5 X = -a |X| = a

Example 4.6.1 Plot the frequency spectrum of signal x(t) shown in Figure 4.6.1(a).

Figure 4.6.1(a)

SOLUTION:

;

Im

Re

(a+jb)

a

b

X

|X|

Page 35: Chapter 4-Fourier Series

And

Amplitude spectrum:

Since , or , it is satisfied magnitude no 3 in Table 4.6.

So the amplitude spectrum is:

and

Phase spectrum:

Since , it is satisfied magnitude no 2 and no 3 in Table 4.6.

And plot the frequency spectrum for n= 0, ±1, ±2, ±3, ±4, ±5.

The plotted amplitude and phase spectrums of signal x (t) are shown in Figure 4.6.1(b)

and in Figure 4.6.1(c).

Figure 4.6.1(b) Amplitude spectrums

n -5 -4 -3 -2 -1 1 2 3 4 5

0 0 0 0 0

0 0 0 0 0

Page 36: Chapter 4-Fourier Series

Figure 4.6.1(c) Phase spectrums

Example 4.6.2 Plot the frequency spectrum of signal x (t) shown in Figure 4.6.2(a).

Figure 4.6.2(a)

SOLUTION:

;

And

Amplitude spectrum:

Since , or , it is satisfied magnitude no 2 in Table 4.6.

So the amplitude spectrum is:

and

Phase spectrum:

Page 37: Chapter 4-Fourier Series

Since , it is satisfied magnitude no 2 and no 3 in Table 4.6.

And plot the frequency spectrum for n= 0, ±1, ±2, ±3, ±4, ±5.

The plotted amplitude and phase spectrums of signal x (t) are shown in Figure 4.6.2(b)

and in Figure 4.6.2(c).

Figure 4.6.2(b) Amplitude spectrums

n -5 -4 -3 -2 -1 1 2 3 4 5

Page 38: Chapter 4-Fourier Series

Figure 4.6.2(c) Phase spectrums

4.7 Trigonometric Fourier Coefficients and Complex Fourier

Coefficients Relationship

, and

Example 4.7.1 Convert the trigonometric Fourier coefficients of signal x (t) of Figure

4.7.1 to complex Fourier coefficient.

Figure 4.7.1

; ; and

SOLUTION:

Thus,

Page 39: Chapter 4-Fourier Series

. This is true for n= 0, ±1, ±2, ±3, …

Thus,

Example 4.7.2 Convert the trigonometric Fourier coefficients of signal x (t) of' Figure

4.7.2 to complex Fourier coefficient.

Figure 4.7.2

; ; and

SOLUTION:

Thus,

. This is true for n= 0, ±1, ±2, ±3…

Page 40: Chapter 4-Fourier Series

Thus,