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Fourier Series Representation of Periodic Signals

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The response of an LTI systems to a complex exponential input is the same ... essentially undistorted and significantly attenuate or eliminate others ... – PowerPoint PPT presentation

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Title: Fourier Series Representation of Periodic Signals


1
Fourier Series Representation of Periodic Signals
2
The Response of LTI Systems to Complex
Exponentials
  • The response of an LTI systems to a complex
    exponential input is the same complex exponential
    with only a change in amplitude

3
The Response of LTI Systems to Complex
Exponentials(2)
  • A signal for which the system output is a
    constant times the input is referred to as an
    eigenfunction of the system , and the amplitude
    factor is referred to as the systems eigenvalue.

4
The Response of LTI Systems to Complex
Exponentials(3)
5
The Response of LTI Systems to Complex
Exponentials(4)
6
The Response of LTI Systems to Complex
Exponentials(5)
7
Example 3.1-1
8
Example 3.1-2
9
Fourier Series Representation of Continuous-Time
Periodic Signals
  • A signal is periodic if

10
Example 3.2
11
Example 3.2(2)
12
F.S. Representation of Continuous-Time Periodic
Signals(2)
  • Suppose that x(t) is real and can be represented
    in
  • then

13
F.S. Representation of Continuous-Time Periodic
Signals(3)
14
F.S. Representation of Continuous-Time Periodic
Signals(4)
15
F.S. Representation of Continuous-Time Periodic
Signals(5)
16
F.S. Representation of Continuous-Time Periodic
Signals(6)
17
Example 3.3
18
Example 3.4
19
Example 3.4(2)
20
Example 3.5
21
Example 3.5(2)
22
Example 3.5(3)
23
Convergence of the Fourier Series
  • Periodic signal x(t) by a linear combination of
    a finite number

24
Convergence of the Fourier Series(2)
  • The energy in the error over one period
  • One class of periodic signals are represent
  • -able through the F.S. those signals which
    have finite energy over a single period

25
Convergence of the Fourier Series(3)
  • Most of the periodic signals we consider do have
    finite energy over a single period, they have
    F.S. representation.

26
Dirichlet conditions 1
  • x(t) must be absolutely integrable

27
Dirichlet conditions 1(2)
  • A periodic signal that violates the first
    Dirichlet conditions

28
Dirichlet conditions 2
  • In any finite interval of time, x(t) is of
    bounded variation that is, there are no more
    than a finite number of maxima and minima during
    any single period of the signal

29
Dirichlet conditions 2(2)
  • An example of a function that meets condition 1
    but not condition 2

30
Dirichlet conditions 3
  • In any finite interval of time, there are only a
    finite number of discontinuities
  • An example of a function that violates Dirichlet
    conditions 3

31
Gibbs phenomenon
  • xN(t) of a discontinuous signal x(t) will in
    general exhibit high-frequency ripples and
    overshoot x(t) near the discontinuous

32
Gibbs phenomenon(2)
33
Properties of Continuous-Time Fourier Series
34
Time Shifting
35
Time Reversal
36
Time Scaling
  • The Fourier coefficients have not changed, the
    Fourier series representation has changed because
    of the change in the fundamental frequency

37
Multiplication
38
Conjugation and Parsevals Relation
  • Conjugation
  • Parsevals relation

39
Example 3.6
40
Example 3.6(2)
41
Example 3.7
42
Example 3.8
43
Example 3.8(2)
44
FS Representation of Discrete-Time Periodic Signal
  • A discrete-time signal xn with period N
  • The set of all discrete-time complex exponential
    signals with period N

45
FS Representation of Discrete-Time Periodic
Signal(2)
  • To consider the representation of more general
    periodic sequences

46
FS Representation of Discrete-Time Periodic
Signal(3)
47
Example 3.10
48
Example 3.11
49
Example 3.11(2)
50
Example 3.12
51
Example 3.12(2)
52
Example 3.12(2)
53
Signal and system
54
3.7 Properties of discrete-time fourier series
  • 3.7.1 Multiplication
  • 3.7.2 First difference
  • 3.7.3 Parsevals relation for discrete-time
    periodic signals
  • 3.7.4 Example

55
3.7.1
  • Multiplication
  • Periodic convolution
  • Aperiodic convolution
  • Ranges form

56
3.7.2
  • First difference
  • Defined as

57
3.7.3
  • Parsevals relation
  • The average power in a periodic signal equals the
    sum of the average powers in all of its harmonic
    components

58
3.7.4
  • Example 3.13

59
3.7.4
60
3.7.4
  • Example 3.14

61
3.7.4
62
3.8 Fourier series and LTI systems
  • Continuous-time LTI system
  • Discrete-time LTI system

63
3.8
  • Continuous-time
  • Special case
  • Discrete-time
  • Focus in

64
3.8
  • Continuous-time
  • Example 3.16

65
3.8
66
3.8
  • Discrete-time
  • Example 3.17

67
3.8
68
3.9 Filtering
  • 3.9.1 Frequency-shaping filters
  • 3.9.2 Frequency-selective filters

69
3.9.1
  • Frequency-shaping filters
  • Linear time-invariant systems that change the
    shape of the spectrum
  • Example

70
3.9.1
71
3.9.2
  • Frequency-selective filters
  • Systems that are designed to pass some
    frequencies essentially undistorted and
    significantly attenuate or eliminate others
  • Example

72
3.9.2
73
3.10 Examples of continuous-time filters
  • 3.10.1 A simple RC lowpass filter
  • 3.10.2 A simple RC highpass filter

74
3.10.1
75
3.10.1
76
3.10.2
77
3.11 Example of discrete-time filters
  • 3.11.1 First-order recursive discrete-time
    filters
  • 3.11.2 Nonrecursive discrete-time filters

78
3.11.1
79
3.11.2
80
3.11.2
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