Title: Review on Fourier
1Review on Fourier
2-
- Slides edited from
- Prof. Brian L. Evans and Mr. Dogu Arifler Dept.
of Electrical and Computer Engineering The
University of Texas at Austin course - EE 313 Linear Systems and Signals Fall
2003
3Fourier Series
4Spectrogram Demo (DSP First)
- Sound clips
- Sinusoid with frequency of 660 Hz (no harmonics)
- Square wave with fundamental frequency of 660 Hz
- Sawtooth wave with fundamental frequency of 660
Hz - Beat frequencies at 660 Hz /- 12 Hz
- Spectrogram representation
- Time on the horizontal axis
- Frequency on the vertical axis
5Frequency Content Matters
- FM radio
- Single carrier at radio station frequency (e.g.
94.7 MHz) - Bandwidth of 165 kHz left audio channel, left
right audio channels, pilot tone, and 1200 baud
modem - Station spacing of 200 kHz
- Modulator/Demodulator (Modem)
6Demands for Broadband Access
Courtesy of Milos Milosevic (Schlumberger)
7DSL Broadband Access Standards
Courtesy of Shawn McCaslin (Cicada Semiconductor,
Austin, TX)
8Multicarrier Modulation
- Discrete Multitone (DMT) modulation
- ADSL (ANSI 1.413) and proposed for VDSL
- Orthogonal Freq. Division Multiplexing (OFDM)
- Digital audio/video broadcasting (ETSI
DAB-T/DVB-T)
Courtesy of Güner Arslan (Cicada Semiconductor)
channel frequency response
magnitude
a carrier
a subchannel
frequency
Harmonically related carriers
9Periodic Signals
- f(t) is periodic if, for some positive constant
T0 - For all values of t, f(t) f(t T0)
- Smallest value of T0 is the period of f(t).
- sin(2pfot) sin(2pf0t 2p) sin(2pf0t 4p)
period 2p. - A periodic signal f(t)
- Unchanged when time-shifted by one period
- Two-sided extent is t ? (-?, ?)
- May be generated by periodically extending one
period - Area under f(t) over any interval of duration
equal to the period is the same e.g.,
integrating from 0 to T0 would give the same
value as integrating from T0/2 to T0 /2
10Sinusoids
- f0(t) C0 cos(2 p f0 t q0)
- fn(t) Cn cos(2 p n f0 t qn)
- The frequency, n f0, is the nth harmonic of f0
- Fundamental frequency in Hertz is f0
- Fundamental frequency in rad/s is w 2 p f0
- Cn cos(n w0 t qn) Cn cos(qn) cos(n w0 t) -
Cn sin(qn) sin(n w0 t) an cos(n w0 t) bn
sin(n w0 t)
11Fourier Series
- General representationof a periodic signal
- Fourier seriescoefficients
- Compact Fourierseries
12Existence of the Fourier Series
- Existence
- Convergence for all t
- Finite number of maxima and minima in one period
of f(t)
13Example 1
- Fundamental period
- T0 p
- Fundamental frequency
- f0 1/T0 1/p Hz
- w0 2p/T0 2 rad/s
14Example 2
- Fundamental period
- T0 2
- Fundamental frequency
- f0 1/T0 1/2 Hz
- w0 2p/T0 p rad/s
15Example 3
- Fundamental period
- T0 2p
- Fundamental frequency
- f0 1/T0 1/2p Hz
- w0 2p/T0 1 rad/s
16Fourier Analysis
17Periodic Signals
- For all t, x(t T) x(t)
- x(t) is a period signal
- Periodic signals havea Fourier
seriesrepresentation - Cn computes the projection (components) of x(t)
having a frequency that is a multiple of the
fundamental frequency 1/T.
18Fourier Integral
- Conditions for the Fourier transform of g(t) to
exist (Dirichlet conditions) - x(t) is single-valued with finite maxima and
minima in any finite time interval - x(t) is piecewise continuous i.e., it has a
finite number of discontinuities in any finite
time interval - x(t) is absolutely integrable
19Laplace Transform
- Generalized frequency variable s s j w
- Laplace transform consists of an algebraic
expression and a region of convergence (ROC) - For the substitution s j w or s j 2 p f to
be valid, the ROC must contain the imaginary axis
20Fourier Transform
- What system properties does it possess?
- Memoryless
- Causal
- Linear
- Time-invariant
- What does it tell you about a signal?
- Answer Measures frequency content
- What doesnt it tell you about a signal?
- Answer When those frequencies occurred in time
21Useful Functions
- Unit gate function (a.k.a. unit pulse function)
- What does rect(x / a) look like?
- Unit triangle function
rect(x)
1
x
0
1/2
-1/2
D(x)
1
x
0
1/2
-1/2
22Useful Functions
- Sinc function
- Even function
- Zero crossings at
- Amplitude decreases proportionally to 1/x
23Fourier Transform Pairs
24Fourier Transform Pairs
F(w) 2 p d(w)
(2p)
w
0
(2p) means that the area under the spike is (2p)
25Fourier Transform Pairs
F(w)
f(t)
(p)
(p)
t
w
w0
-w0
0
0
26Fourier Transform Pairs
sgn(t)
1
-1
27Fourier Transform Properties
28Fourier vs. Laplace Transform Pairs
Assuming that Rea gt 0
29Duality
- Forward/inverse transforms are similar
- Example rect(t/t) ? t sinc(w t / 2)
- Apply duality t sinc(t t/2) ? 2 p
rect(-w/t) - rect() is even t sinc(t t /2) ? 2 p
rect(w/t)
f(t)
1
t
0
t/2
-t/2
30Scaling
- Same as Laplacetransform scaling property
- a gt 1 compress time axis, expand frequency
axis - a lt 1 expand time axis, compress frequency
axis - Effective extent in the time domain is inversely
proportional to extent in the frequency domain
(a.k.a bandwidth). - f(t) is wider ? spectrum is narrower
- f(t) is narrower ? spectrum is wider
31Time-shifting Property
- Shift in time
- Does not change magnitude of the Fourier
transform - Does shift the phase of the Fourier transform by
-wt0 (so t0 is the slope of the linear phase)
32Frequency-shifting Property
33Modulation
34Modulation
- Example y(t) f(t) cos(w0 t)
- f(t) is an ideal lowpass signal
- Assume w1 ltlt w0
- Demodulation is modulation followed by lowpass
filtering - Similar derivation for modulation with sin(w0 t)
Y(w)
1/2 F(ww0)
1/2 F(w-w0)
1/2
w
-w0 - w1
-w0 w1
w0 - w1
w0 w1
0
-w0
w0
35Time Differentiation Property
- Conditions
- f(t) ? 0, when t ? ?
- f(t) is differentiable
- Derivation of propertyGiven f(t) ? F(w)
36Time Integration Property
37Summary
- Definition of Fourier Transform
- Two ways to find Fourier Transform
- Use definitions
- Use properties