Fourier Transformation fx Fourier Transformasjon Fu 1 Continuous











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![Inverse Fourier Transform [1/3] Theorem: Proof: 14 Inverse Fourier Transform [1/3] Theorem: Proof: 14](https://slidetodoc.com/presentation_image_h2/62c5fb459cd8aaaa5826843c4c7939ee/image-14.jpg)
![Inverse Fourier Transform [2/3] Theorem: Proof: 15 Inverse Fourier Transform [2/3] Theorem: Proof: 15](https://slidetodoc.com/presentation_image_h2/62c5fb459cd8aaaa5826843c4c7939ee/image-15.jpg)
![Inverse Fourier Transform [3/3] 16 Inverse Fourier Transform [3/3] 16](https://slidetodoc.com/presentation_image_h2/62c5fb459cd8aaaa5826843c4c7939ee/image-16.jpg)



![Even and Odd Functions [1/3] Def Every function can be split in an even Even and Odd Functions [1/3] Def Every function can be split in an even](https://slidetodoc.com/presentation_image_h2/62c5fb459cd8aaaa5826843c4c7939ee/image-20.jpg)
![Even and Odd Functions [2/3] 1. 2. 3. Even component in f produces an Even and Odd Functions [2/3] 1. 2. 3. Even component in f produces an](https://slidetodoc.com/presentation_image_h2/62c5fb459cd8aaaa5826843c4c7939ee/image-21.jpg)
![Even and Odd Functions [3/3] 22 Even and Odd Functions [3/3] 22](https://slidetodoc.com/presentation_image_h2/62c5fb459cd8aaaa5826843c4c7939ee/image-22.jpg)



























- Slides: 49
Fourier Transformation f(x) Fourier Transformasjon F(u) 1
Continuous Fourier Transform Def The Fourier transform of a one-dimentional function f(x) The Inverse Fourier Transform 2
Continuous Fourier Transform Def - Notation The Fourier transform of a one-dimentional function f(x) The inverse Fourier Transform of F(u) 3
Continuous Fourier Transform Alternative Def 4
Continuous Fourier Transform Example - cos(2 ft) 5
Continuous Fourier Transform Example - cos( t) 6
Continuous Fourier Transform Example - sin( t) 7
Continuous Fourier Transform Example - Delta-function 8
Continuous Fourier Transform Example - Gauss function 9
Signals and Fourier Transform Frequency Information FT FT FT 10
Stationary / Non-stationary signals Stationary FT Non stationary FT The stationary and the non-stationary signal both have the same FT. FT is not suitable to take care of non-stationary signals to give information about time. 11
Transient Signal Frequency Information Constant function in [-3, 3]. Dominating frequency = 0 and some freequency because of edges. Transient signal resulting in extra frequencies > 0. Narrower transient signal resulting in extra higher frequencies pushed away from origin. 12
Transient Signal No Information about Position Moving the transient part of the signal to a new position does not result in any change in the transformed signal. Conclusion: The Fourier transformation contains information of a transient part of a signal, but only the frequency not the position. 13
Inverse Fourier Transform [1/3] Theorem: Proof: 14
Inverse Fourier Transform [2/3] Theorem: Proof: 15
Inverse Fourier Transform [3/3] 16
Properties 17
Fourier Transforms of Harmonic and Constant Function 18
Fourier Transforms of Some Common Functions 19
Even and Odd Functions [1/3] Def Every function can be split in an even and an odd part and each of this can in turn be split in a real and an imaginary part 20
Even and Odd Functions [2/3] 1. 2. 3. Even component in f produces an even component in F Odd component in f produces an odd component in F Oddcomponent in f produces an coefficient -j 21
Even and Odd Functions [3/3] 22
The Shift Theorem 23
The Similarity Theorem 24
The Convolution Theorem 25
Convolution Edge detection 26
The Adjoint of the Fourier Transform Theorem: Suppose f and g er are square integrable. Then: Proof: 27
Plancherel Formel - The Parselval’s Theorem: Suppose f and g are square integrable. Then: Proof: 28
The Rayleigh’s Theorem Conservation of Energy The energy of a signal in the time domain is the same as the energy in the frequency domain 29
The Fourier Series Expansion u a discrete variable - Forward transform Suppose f(t) is a transient function that is zero outside the interval [-T/2, T/2] or is considered to be one cycle of a periodic function. We can obtain a sequence of coefficients by making a discrete variable and integrating only over the interval. 30
The Fourier Series Expansion u a discrete variable - Inverse transform The inverse transform becomes: 31
The Fourier Series Expansion cn coefficients 32
The Fourier Series Expansion zn, an, bn coefficients 33
The Fourier Series Expansion an, bn coefficients 34
Fourier Series Pulse train approximated by Fourier Serie N=1 N=2 N=5 N = 10 35
Fourier Series Pulse train – Java program 36
Pulse Train approximated by Fourier Serie f(x) square wave (T=2) N=1 N=2 N=10 37
Fourier Series Zig tag approximated by Fourier Serie N=1 N=2 N=5 N = 10 38
Fourier Series Negative sinus function N=1 Negative sinus function approximated by Fourier Serie N=2 N=5 N = 10 39
Fourier Series Truncated sinus function N=1 Truncated sinus function approximated by Fourier Serie N=2 N=5 N = 10 40
Fourier Series Line approximated by Fourier Serie N=1 N=2 N=5 41 N = 10 N = 50
Fourier Series Java program for approximating Fourier coefficients Approximate functions by adjusting Fourier coefficients (Java program) 42
The Discrete Fourier Transform - DFT Discrete Fourier Transform - Discretize both time and frequency Continuous Fourier transform Discrete frequency Fourier Serie Discrete frequency and time Discrete Fourier Transform 43
The Discrete Fourier Transform - DFT Discrete Fourier Transform - Discretize both time and frequency { fi } sequence of length N, taking samples of a continuous function at equal intervals 44
Continuous Fourier Transform in two Dimensions Def The Fourier transform of a two-dimentional function f(x, y) The Inverse Fourier Transform 45
The Two-Dimensional DFT and Its Inverse 46
Fourier Transform in Two Dimensions Example 1 47
Fourier Transform in Two Dimensions Example 2 48
End 49