ee313 linear systems and signals fall 2010 initial conversion of content to powerpoint by dr. wade...
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EE313 Linear Systems and Signals Fall 2010
Initial conversion of content to PowerPointby Dr. Wade C. Schwartzkopf
Prof. Brian L. Evans
Dept. of Electrical and Computer Engineering
The University of Texas at Austin
Fourier Series
11 - 2
Course Outline• Time domain analysis (lectures 1-10)
Signals and systems in continuous and discrete timeConvolution: finding system response in time domain
• Frequency domain analysis (lectures 11-16)
Fourier seriesFourier transformsFrequency responses of systems
• Generalized frequency domain analysis (lectures 17-26)
Laplace and z transforms of signalsTests for system stabilityTransfer functions of linear time-invariant systems
Roberts, ch. 1-3
Roberts, ch. 4-7
Roberts, ch. 9-12
11 - 3
Periodic Signals• For some positive constant T0
f(t) is periodic if f(t) = f(t + T0) for all values of t (-, )
Smallest value of T0 is the period of f(t)
• A periodic signal f(t)Unchanged when time-shifted by one period
May be generated by periodically extending one period
Area under f(t) over any interval of duration equal to the period is same; e.g., integrating from 0 to T0 would give the same value as integrating from –T0/2 to T0 /2
00
0000
12sin
2
22sin)22sin()2sin(
ftf
ftftftf
11 - 4
Sinusoids• Fundamental f1(t) = C1 cos(2 f0 t + )
Fundamental frequency in Hertz is f0
Fundamental frequency in rad/s is = 2 f0
• Harmonic fn(t) = Cn cos(2 n f0 t + n)
Frequency, n f0, is nth harmonic of f0
• Magnitude/phase and Cartesian representations Cn cos(n 0 t + n) =
Cn cos(n) cos(n 0 t) - Cn sin(n) sin(n 0 t) = an cos(n 0 t) + bn sin(n 0 t)
11 - 5
Fourier Series• General representation
of a periodic signal
• Fourier seriescoefficients
• Compact Fourierseries
1
000 sincosn
nn tnbtnaatf
n
nn
nnn
nnn
a
b
bacac
tncctf
1
2200
100
tan
and, , where
cos
0
0
0
0 00
0 00
00
0
sin2
cos2
1
T
n
T
n
T
dttntfT
b
dttntfT
a
dttfT
a
11 - 6
Existence of the Fourier Series• Existence
• Convergence for all t
• Finite number of maxima and minima in one period of f(t)
• What about periodic extensions of
0
0
Tdttf
ttf
1 1-for 1
tt
tg 10for 1
sin
t
tts
11 - 7
Example #1
• Fundamental periodT0 =
• Fundamental frequencyf0 = 1/T0 = 1/ Hz
0 = 2/T0 = rad/s
0
A
f(t)
-A
,15,11,7,38
,13,9,5,18
even is 0
22
22
nn
A
nn
An
bn
2/3
2/1
2/1
2/1
0
10
) sin( ) 22(
) sin( 2
symmetric) odd isit (because 0
plot) theof inspection(by 0
sin) cos(
dttnπtAA
dttnπtAb
a
a
tnπbtnπaatf
n
n
nnn
11 - 8
Example #2
• Fundamental periodT0 =
• Fundamental frequencyf0 = 1/T0 = 1/( Hz
0 = 2/T0 = 1 rad/s
,15,11,7,3
,15,11,7,3 allfor 0
odd
2even 0
2
10
n
n
nn
nC
C
n
n
1
f(t)