16
Image Enhancement in Frequency Domain Nana Ramadijanti Laboratorium Computer Vision Politeknik Elekltronika Negeri Surabaya PENS-ITS 2009

Image Enhancement in Frequency Domain

  • Upload
    niran

  • View
    94

  • Download
    0

Embed Size (px)

DESCRIPTION

Image Enhancement in Frequency Domain. Nana Ramadijanti Laboratorium Computer Vision Politeknik Elekltronika Negeri Surabaya PENS-ITS 2009. Image and Its Fourier Spectrum. Basic Steps Multiply pixel f(x,y) of the input image by (-1) x+y . Compute F(u,v), the DFT G(u,v)=F(u,v)H(u,v) - PowerPoint PPT Presentation

Citation preview

Image Enhancement in Frequency Domain

Nana RamadijantiLaboratorium Computer Vision

Politeknik Elekltronika Negeri Surabaya PENS-ITS2009

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Image and Its Fourier Spectrum

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Filtering in Frequency Domain: Basic Steps

Basic Steps1. Multiply pixel f(x,y) of the

input image by (-1)x+y. 2. Compute F(u,v), the DFT3. G(u,v)=F(u,v)H(u,v)4. g1(x,y)=F-1{G(u,v)}5. g(x,y) = g1(x,y)*(-1)x+y

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Notch Filter

• The frequency response F(u,v) has a notch at origin (u = v = 0).

• Effect: reduce mean value.

• After post-processing where gray level is scaled, the mean value of the displayed image is no longer 0.

.1

00),(

otherwisevu

vuF

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Low-pass & High-pass Filtering

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Gaussian Filters

• Fourier Transform pair of Gaussian function

• Depicted in figures are low-pass and high-pass Gaussian filters, and their spatial response, as well as FIR masking filter approximation.

• High pass Gaussian filter can be constructed from the difference of two Gaussian low pass filters.

222

22

2

2/

2)()(

x

u

AexhAeuH

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Gaussian Low Pass Filters

D(u,v): distance from the origin of Fourier transform

2

2

2),(exp),(

vuDvuH

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Ideal Low Pass Filters

• The cut-off frequency Do determines % power are filtered out.

• Image power as a function of distance from the origin of DFT (5, 15, 30, 80, 230)

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Effects of Ideal Low Pass Filters

• Blurring can be modeled as the convolution of a high resolution (original) image with a low pass filter.

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Ringing and Blurring

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Butterworth Low Pass Filters

noDvuDvuH 2/),(1

1),(

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

• Ideal high pass filter

• Butterworth high pass filter

• Gaussian high pass filter

High Pass Filters

.1

),(0),(

otherwiseDvuDif

vuH o

nvuDDvuH 2

0 ),(/11),(

2

0

2

2),(exp1),(

DvuDvuH

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Applications of HPFs

• Ideal HPF– Do = 15, 30, 80

• Butterworth HPF– n = 2,– Do = 15, 30, 80

• Gaussian HPF– Do = 15, 30, 80

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya PENS-ITS

Laplacian HPF

• 3D plots of the Laplacian operator,

• its 2D images, • spatial domain response

with center magnified, and• Compared to the FIR mask

approximation

),(2/2/

),(22

2

vuFNvMu

yxf

SekilaS InfO

Ada beberapa hal yang harus dikuasai sebelum menguasai materi di dalam image processing yaitu: matematika, aljabar, pengolahan sinyal,

statistik dan pemrograman.

BergaBunglah denGan Kami

Laboratorium Computer VisionPoliteknik Elektronika Negeri Surabaya

PENS-ITS 2009