review of fourier series - georgia institute of...
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunication Systems
Review of Fourier Series
ECPE 3614Lecture 2
Instructor: Gregory D. Durgin
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L22
Outline of Lecture
§Review of Lecture 1§Calculation of Fourier Coefficients§Trigonometric vs. Complex FS§Example 1: Triangular Waveform§Example 2: Sawtooth Waveform§Example 3: Rectangular Waveform
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L23
Review
§Fourier’s Theorem: All real periodic functionsmay be expressed as a linear combination ofharmonic sinusoids.§There are two types of Fourier Series:§ Trigonometric Fourier Series – uses a series sines and
cosines.§ Complex Fourier Series – uses a series of complex
exponentials as oscillators.§ These series are just two different ways of doing the
same thing.
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L24
The Trigonometric FourierSeries
§Mathematically, the trigonometric Fourier seriesmay be written in this form:
§Note that the n=0 case for the sine summation isnot important since the term drops out to zero
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L25
Calculating TrigonometricFourier Series Coefficients
Let’s say we want to calculate the mth cosine coefficient, am.How do we go about it? First, start with the definition of thetrig. FS:
Step 1: multiply both sides by the mth harmonic cosine asshown below:
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L26
Calculating TrigonometricFourier Coefficients
Step 2: Integrate both sides over exactly one period of theperiodic function. (This is starting to look complicated, butwe can simplify in a few steps.)
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L27
Calculating TrigonometricFourier Coefficients
Step 3: The right-side integral may be distributed across eachterm in the series summation:
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L28
Calculating TrigonometricFourier Coefficients
Step 4: Take a look and the cos-sin integral:
This is a standard definite integral that can be found in manybooks. Since this is an integration of a harmonic sine wave (nis an integer) and a harmonic cosine wave (m is an integer)over exactly one period, T, the integral always evaluates to 0.
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L29
Calculating TrigonometricFourier Coefficients
Step 5: There are 3 possible outcomes for the cos-cos definiteintegral:
§m and n are different: the integral always evaluates to 0.§m and n are the same (but not 0): the integral evaluates to
T/2.§m and n are 0: the integral evaluates to T.
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L210
Calculating TrigonometricFourier Coefficients
Step 6: Good news! Based on the definite integrations ofsteps 4 and 5, all but one of the terms will vanish.
always 0
always 0 except forthe case m=n.
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L211
Calculating TrigonometricFourier Coefficients
Step 7: For the case of m>0, the results of our hard effortsproduces an equation for am:
Just switch the m to an n (to keep notation consistent) andrearrange the equation to solve for an. Now we have theformula for the nth cosine Fourier coefficient!
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L212
Calculating TrigonometricFourier Coefficients
Step 8: One last step – for the case of m=0, the results of ourhard efforts produces an equation for a0:
Rearranging, the equation for a0 becomes…
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L213
Calculating the TrigonometricFourier Coefficients…
The full set of trigonometricFourier coefficients is shown on theright. The derivation for the bn isidentical to the an, except that asine term is used in Step 1. Note:the limits of integration for theseformulas are somewhat arbitrary.Since the integrands are periodicfunctions, any integration lengththat spans exactly one period, T,will produce the correct result.
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L214
Example of Trig FS:A Triangular Waveform
§Blackboard Example: Find the trigonometric Fouriercoefficients for this triangular waveform with period of 1s.
time, t
+1/2
1 s
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L215
The Complex Fourier Series
§Below is the complex Fourier Series:
§Key points about the complex series:§ unlike an and bn, cn may be a complex number.§ summation limits are from –infinity to +infinity.§ if f(t) is to be a real-valued function, the complex
Fourier coefficients must have special properties (seeHomework 1, problem 1).
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L216
Calculating The ComplexFourier Coefficients
Start with the definition of the complex Fourier Coefficients:
Step 1: To calculate the mth coefficient, multiply both sidesof the equation by the –mth complex exponential harmonic:
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L217
Calculating The ComplexFourier Coefficients
Step 2: Integrate both sides over an entire period, T.
Note: The imaginary j does not change how you performintegration. Just take it along for the ride, as if it were aconstant.
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L218
Calculating The ComplexFourier Coefficients
Step 3: Distribute the integral to each term inside thesummation. This step is valid because integration is linear.
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L219
Calculating The ComplexFourier Coefficients
Step 4: Study the following integral:
Since this is an integration of complex harmonic sinusoids(the value n-m is an integer) over exactly one period, theresult is only non-zero for m=n. For m=n, the integralevaluates to T.
0 unless m=n
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L220
Calculating The ComplexFourier Coefficients
Step 5: After all of the zero terms are removed, the finalresult is given below:
Swapping the letter m for n (for consistency of notation) andre-arranging provides us the formula for the complex Fouriercoefficients:
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L221
The Complex Fourier Series
Below is the integral for calculating complex Fourier coefficients.The drawback to this method is the integration of the complexexponent. This integration often produces a complex coefficientfor cn. One nice advantage: only one formula as opposed to the 3equations required for the trigonometric series.
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L222
To Convert from Complex FSto Trig FS Coefficients…
… just make the followingsubstitutions. This cansave a lot of computation!
Remember: the complex Fourier series is justa different way to keep track of the spectral
decomposition.
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L223
To Convert from Trig FS toComplex FS Coefficients…
… just make the followingsubstitutions.
The set of harmonic sinusoids (both complexexponential and trigonometric) are said to be abasis that spans the set of real periodic functions.
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L224
Ex. 1: Triangular Waveform
time, t
+1/2
1 s
Trig FS coefficients:
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Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L225
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Triangle Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 0
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L226
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Triangle Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 1
14
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L227
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Triangle Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 3
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L228
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Triangle Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 5
15
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L229
Ex. 2: The SawtoothWaveform
Trig FS coefficients:
time, t
+1/2
-1/2
1 s
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L230
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Sawtooth Waveform of T=1
time, t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 1
16
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L231
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Sawtooth Waveform of T=1
time, t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 3
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L232
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Sawtooth Waveform of T=1
time, t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 6
17
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L233
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Sawtooth Waveform of T=1
time, t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 15
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L234
Ex. 3: The RectangularWaveform
Trig FS coefficients:
time, t
+1/2
1 s
18
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L235
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Rectangular Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 1
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L236
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Rectangular Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 3
19
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L237
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Rectangular Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 5
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L238
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Rectangular Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 7
20
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L239
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Rectangular Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 13
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L240
-2 -1.5 -1 -0.5 0 0.5 1 1.5 2-0.5
0
0.5
1Rectangular Waveform of T=1
time,t
Sig
nal A
mpl
itude
Exact SignalFourier Series through term 25
21
Copyright Gregory D. Durgin 2000VIRGINIA POLYTECHNIC INSTITUTEAND STATE UNIVERSITY
TechVirginia
1 8 7 2
ECPE 3614 Introduction toCommunications Systems
L241
Key Points of Lecture
§Basic Form of the Fourier Series§Calculate Trigonometric Fourier Coefficients§Calculate Complex Fourier Coefficients§Convert Between Complex and Trig Fourier
Coefficients§Examples of how truncated Fourier Series
approximate real signals with increasing accuracy