Fourier Series: Deriving and Finding Coefficients - Prof. Alexander Parlos, Study notes of Mechanical Engineering

The process of deriving the fourier series for a given function and finding the fourier coefficients for a discrete function. It includes detailed calculations and explanations using integrals and discrete summations. This information is essential for students and researchers in the field of electrical engineering, physics, and mathematics, particularly those focusing on signal processing and data analysis.

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Pre 2010

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364 Recitation Notes
9/5/2007
EXAMPLE 1.
Derive the Fourier Series of the following function:
First Identify the function:
( ) 1 , x*T t T+x*T, x= ...,-2,-1,0,1,2,...
t
F t for
T
Then plug this equation into the Fourier transform equation:
0
1 1
( ) (1 )
o o
T
jw kt jw kt
k
T
t
c F t e dt e
T T T
Integrating over one period. Solving for co:
0
0 0
2
1 1
(1 ) (1 )
1 1
( )
2 2
o
T T
jkw
o
o
t t
c e dt dt
T T T T
t
c T
T T
Continue solving for the series coefficients:
0 0 0
1 1 1
(1 ) o o o
T T T
jw kt jw kt jw kt
k
t t
T T T T T
Solving the first integral:
1
T
t
F(t)
pf3

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364 Recitation Notes

9/5/

EXAMPLE 1.

Derive the Fourier Series of the following function:

First Identify the function:

( ) 1 , xT t T+xT, x= ...,-2,-1,0,1,2,...

t F t for T

   

Then plug this equation into the Fourier transform equation:

0

o o

T jw kt jw kt k T

t c F t e dt e T T T

    

Integrating over one period. Solving for co:

0

0 0

2

o

T (^) jkw T

o

o

t t c e dt dt T T T T

t c T T T

    

Continue solving for the series coefficients:

0 0 0

o o o

T T T jw kt jw kt jw kt k

t t

c e e dt e dt

T T T T T

  

  

Solving the first integral:

1

T

t

F(t)

  0 0 0 0

o o o

T jw kt jw kt T jw kT

e dt e e

T T jw k T jw k

 ^  ^ ^  

To solve the second integral us integrate by parts:

0

2 0 0

2

o

o

o

o o

o o

T jw kt

jw kt

jw kt

o

jw kt T^ T jw kt

o o

jw kT jw kt

o o

t e dt T T

u t dv e

e du v jw k

e e u dv uv v du t dt T jw k jw k

Te e jw kT jw k

 

 

    ^  

  

Adding this result to the result of the first integral:

 

 

2 0

2 0

2 2 2 0 0

o o o

o

o

jw kT jw kT jw kt k o o

jw kt k o o

jw kt k

c e Te e T jw k jw kT jw k

c e T jw k jw kT jw k

c e Tjw k T w k

  

 ^    
 ^    

since (^0)

2 w T

  ck becomes:

2

jw kt o

ck e

j  k k

This result is then plugged into the Fourier series:

1 2 2

1

j kt j kt T T k k k k

c e c e

   

 

 ^ 