Fourier Filters in Image Analysis: Understanding Continuous and Discrete Transformations
Learn about Continuous and Discrete Fourier Transforms, Convolution Theorems, and Circular Filters in Image Analysis. Explore how to apply Fourier filter techniques effectively.
Fourier Filters in Image Analysis: Understanding Continuous and Discrete Transformations
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Presentation Transcript
IMAGE ANALYSIS CHAPTER 8 Fourier Filters A. Dermanis
Continuous Fouriertransform f(x,y) F(u,v) + + Continuous inverse Fouriertransform F(u,v) = f(x,y) e–i2(ux+vy)dxdy un vm –i 2 (+ ) 1 – – N M Fuv = fnm e NM NM NM + + Discrete Fouriertransform f(x,y) = F(u,v) ei2(ux+vy)dxdy fij Fuv n=1 m=1 u=1 v=1 – – Discrete inverse Fouriertransform un vm i 2 (+ ) fnm = Fuv e N M Continuous and discrete Fouriertransform in two dimensions A. Dermanis
g(x) = h(–x) f() d f(x)h(x) + – gij = hi–n,j–mfnm = hnmfi–n,j–m ++ ++ n = –m = – n = –m = – f(x) F() g(x) G() h(x) H() Continuous convolution theorem G(u) = F(u)H(u) fij Fuv gij Guv hij Huv Discrete convolution theorem {gij} = {hij}{fij} Guv = HuvFuv A. Dermanis
gij = hi–n,j–mfnm ++ n = –m = – Discrete convolution theorem {fij} {Fuv} DFT convolution multiplication Guv = Huv Fuv inverse DFT {gij} {Guv} A. Dermanis
Circular Filters High Pass Low Pass 1 0 1 0 1 1 A. Dermanis
An example of Fourier filtering with circular filters Original Fourier transform After circular high-pass filter, R = 50 After circular low-pass filter, R = 100 After circular low-pass filter, R = 75 After circular low-pass filter, R = 50 A. Dermanis