fourier transform
DESCRIPTION
yaTRANSCRIPT
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ContentsComplex numbers etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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IntroductionJean Baptiste Joseph Fourier (*1768-1830)French MathematicianLa Thorie Analitique de la Chaleur (1822) *
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Fourier SeriesAny periodic function can be expressed as a sum of sines and/or cosinesFourier Series*
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Fourier TransformEven functions that are not periodic have a finite area under curvecan be expressed as an integral of sines and cosines multiplied by a weighing functionBoth the Fourier Series and the Fourier Transform have an inverse operation:Original Domain Fourier Domain*
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ContentsComplex numbers etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Complex numbersComplex number
Its complex conjugate*
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Complex numbers polarComplex number in polar coordinates*
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Eulers formula*Sin ()Cos ()??
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*ReImVector
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Complex mathComplex (vector) addition
Multiplication with I is rotation by 90 degrees*
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Unit impulse (Dirac delta function)Definition
Constraint
Sifting property
Specifically for t=0*
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Discrete unit impulseDefinition
Constraint
Sifting property
Specifically for x=0*
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What does this look like?Impulse train*T = 1
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Fourier Series
with*Series of sines and cosines, see Eulers formula
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Fourier TransformContinuous Fourier Transform (1D) Inverse Continuous Fourier Transform (1D)
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*Symmetry: The only difference between the Fourier Transform and its inverse is the sign of the exponential.
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Fourier
Euler
Fourier and Euler*
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If f(t) is real, then F() is complexF() is expansion of f(t) multiplied by sinusoidal termst is integrated over, disappearsF() is a function of only , which determines the frequency of sinusoidalsFourier transform frequency domain*
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Examples Block 1*-W/2W/2A
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Examples Block 2*
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Examples Block 3*?
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Examples Impulse*
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Examples Shifted impulse*
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Examples Shifted impulse 2*Real partImaginary partimpulseconstant
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Examples - Impulse train*
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Examples - Impulse train 2*
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Intermezzo: Symmetry in the FT*
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*
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Fourier + ConvolutionWhat is the Fourier domain equivalent of convolution?*
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What is*
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Intermezzo 1What is ?
Let , so *
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Intermezzo 2
Property of Fourier Transform*
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Fourier + Convolution contd*
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Recapitulation 1Convolution in one domain is multiplication in the other domain
And (see book)
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Recapitulation 2Shift in one domain is multiplication with complex exponential in the other domain
And (see book)*
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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SamplingSampled function can be written as
Obtain value of arbitrary sample k as*
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Sampling - 2*
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Sampling - 3*
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Sampling - 4*
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FT of sampled functionsFourier transform of sampled function
Convolution theorem
From FT of impulse train*(who?)
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FT of sampled functions
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Sifting property*
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Sampling theoremBand-limited function
Sampled functionlower value of 1/T would cause triangles to merge*
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Sampling theorem 2Sampling theorem:If copy of can be isolated from the periodic sequence of copies contained in , can be completely recovered from the sampled version.Since is a continuous, periodic function with period 1/T, one complete period from is enough to reconstruct the signal.This can be done via the Inverse FT. *
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Extracting a single period from that is equal to is possible if Sampling theorem 3*
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Aliasing
If , aliasing can occur *
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Discrete Fourier TransformFourier Transform of a sampled function is an infinite periodic sequence of copies of the transform of the original continuous function*
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Discrete Fourier TransformContinuous transform of sampled function*
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is discrete function is continuous and infinitely periodic with period 1/T *
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We need only one period to characteriseIf we want to take M equally spaced samples from in the period = 0 to = 1/, this can be done thus *
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Substituting
Into
yields*
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ContentsComplex number etc.ImpulsesFourier Transform (+examples)Convolution theoremFourier Transform of sampled functionsSampling theoremAliasingDiscrete Fourier TransformApplication Examples*
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Fourier Transform Table*
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*
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Formulation in 2D spatial coordinatesContinuous Fourier Transform (2D) Inverse Continuous Fourier Transform (2D) with angular frequencies*
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ContentsFourier Transform of sine and cosine2D Fourier TransformProperties of the Discrete Fourier Transform
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Eulers formula*
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*Recall
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*Recall
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*Cos(t)Sin(t)1/21/2i
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ContentsFourier Transform of sine and cosine2D Fourier TransformProperties of the Discrete Fourier Transform*
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Formulation in 2D spatial coordinatesContinuous Fourier Transform (2D) Inverse Continuous Fourier Transform (2D) with angular frequencies*
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Discrete Fourier TransformForward
Inverse*
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Formulation in 2D spatial coordinatesDiscrete Fourier Transform (2D) Inverse Discrete Transform (2D) *
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Spatial and Frequency intervalsInverse proportionality(Smallest) Frequency step depends on largest distance covered in spatial domainSuppose function is sampled M times in x, with step , distance is covered, which is related to the lowest frequency that can be measured *
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Examples*
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Fourier Series
with*Series of sines and cosines, see Eulers formula
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Examples*
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Periodicity2D Fourier Transform is periodic in both directions*
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Periodicity2D Inverse Fourier Transform is periodic in both directions*
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Fourier Domain*
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Inverse Fourier DomainPeriodic?*Periodic!
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ContentsFourier Transform of sine and cosine2D Fourier TransformProperties of the Discrete Fourier Transform*
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Properties of the 2D DFT*
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*RealImaginarySin (x)Sin (x + /2)Real
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*RealImaginaryF(Cos(x))F(Cos(x)+k)Even
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*RealOddSin (x)Sin(y)Sin (x)Imaginary
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*RealImaginary(Sin (x)+1)(Sin(y)+1)
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Symmetry: even and oddAny real or complex function w(x,y) can be expressed as the sum of an even and an odd part (either real or complex)*
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PropertiesEven function
Odd function*
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Properties - 2*
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Consequences for the Fourier TransformFT of real function is conjugate symmetric
FT of imaginary function is conjugate antisymmetric*
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*Im
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*Re
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*Re
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*Im
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FT of even and odd functionsFT of even function is real
FT of odd function is imaginary*
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*RealImaginaryCos (x)Even
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*RealImaginarySin (x)Odd
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