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Fourier Transforms
The Fourier Transform is a mathematical technique that transforms a
function of time to a function of frequency. It is closely related to
the Fourier Series. The Fourier transform of a function of time is
a complex-valued function of frequency, whose magnitude
(absolute value) represents the amount of that frequency
present in the original function, and whose argument is
the phase offset of the basic sinusoid in that frequency. The
Fourier transform is not limited to functions of time, but
the domain of the original function is commonly referred to
as the time domain. There is also an inverse Fourier
transform that mathematically synthesizes the original
function from its frequency domain representation, as proven
by the Fourier inversion theorem.
( )
f x
( )
1
( ) ( )
2
is x t
f x f t e dt ds

 

 
  
)
1 1
( )
2 2
isx ist
e f t e dt ds
 
 

 
 
  
 
 
1
( ) ( ) (1)
2
ist
F s f t e dt




      

1
( ) ( ) (2)
2
isx
f x F s e ds



     

Consider the Fourier integral representation of the function
given by
Let
Then
( )
f x
 
( ) .
F f x
The integral defined by (1) is called the Fourier transform of the function
and is denoted by
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FT full.pptx .

  • 1. Fourier Transforms The Fourier Transform is a mathematical technique that transforms a function of time to a function of frequency. It is closely related to the Fourier Series. The Fourier transform of a function of time is a complex-valued function of frequency, whose magnitude (absolute value) represents the amount of that frequency present in the original function, and whose argument is the phase offset of the basic sinusoid in that frequency. The Fourier transform is not limited to functions of time, but the domain of the original function is commonly referred to as the time domain. There is also an inverse Fourier transform that mathematically synthesizes the original function from its frequency domain representation, as proven by the Fourier inversion theorem.
  • 2. ( ) f x ( ) 1 ( ) ( ) 2 is x t f x f t e dt ds          ) 1 1 ( ) 2 2 isx ist e f t e dt ds                 1 ( ) ( ) (1) 2 ist F s f t e dt             1 ( ) ( ) (2) 2 isx f x F s e ds           Consider the Fourier integral representation of the function given by Let Then ( ) f x   ( ) . F f x The integral defined by (1) is called the Fourier transform of the function and is denoted by
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