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Page 1 Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_1.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT The Lecture Contains: Fourier analysis Discrete Fourier Transform (DFT) Properties Coefficients Dimensionality reduction Discrete Cosine Transform (DCT) Page 2 Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_1.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT The Lecture Contains: Fourier analysis Discrete Fourier Transform (DFT) Properties Coefficients Dimensionality reduction Discrete Cosine Transform (DCT) Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_2.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT Fourier analysis Fourier analysis represents a periodic wave as a sum of (infinite) sine and cosine waves Way to analyze the frequency components in a signal Fourier transform is a transformation from time domain to frequency domain can be obtained from g(u) by the inverse transformation and form a Fourier transform pair Page 3 Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_1.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT The Lecture Contains: Fourier analysis Discrete Fourier Transform (DFT) Properties Coefficients Dimensionality reduction Discrete Cosine Transform (DCT) Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_2.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT Fourier analysis Fourier analysis represents a periodic wave as a sum of (infinite) sine and cosine waves Way to analyze the frequency components in a signal Fourier transform is a transformation from time domain to frequency domain can be obtained from g(u) by the inverse transformation and form a Fourier transform pair Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_3.htm[6/14/2012 3:53:54 PM] Module 7:Data Representation Lecture 34: DFT and DCT Discrete Fourier Transform (DFT) For discrete case, assume vector x has N components DFT of x, denoted by X, has N components given by Inverse transformation (IDFT) is given by To avoid using separate scaling factors, both can be taken as Page 4 Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_1.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT The Lecture Contains: Fourier analysis Discrete Fourier Transform (DFT) Properties Coefficients Dimensionality reduction Discrete Cosine Transform (DCT) Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_2.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT Fourier analysis Fourier analysis represents a periodic wave as a sum of (infinite) sine and cosine waves Way to analyze the frequency components in a signal Fourier transform is a transformation from time domain to frequency domain can be obtained from g(u) by the inverse transformation and form a Fourier transform pair Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_3.htm[6/14/2012 3:53:54 PM] Module 7:Data Representation Lecture 34: DFT and DCT Discrete Fourier Transform (DFT) For discrete case, assume vector x has N components DFT of x, denoted by X, has N components given by Inverse transformation (IDFT) is given by To avoid using separate scaling factors, both can be taken as Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_4.htm[6/14/2012 3:53:54 PM] Module 7:Data Representation Lecture 34: DFT and DCT Properties Parseval's theorem: , i.e., length of vectors is preserved When both scaling factors are Contractive mapping Invertible, linear transformation Essentially, a rotation in N-dimensional space Page 5 Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_1.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT The Lecture Contains: Fourier analysis Discrete Fourier Transform (DFT) Properties Coefficients Dimensionality reduction Discrete Cosine Transform (DCT) Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_2.htm[6/14/2012 3:53:53 PM] Module 7:Data Representation Lecture 34: DFT and DCT Fourier analysis Fourier analysis represents a periodic wave as a sum of (infinite) sine and cosine waves Way to analyze the frequency components in a signal Fourier transform is a transformation from time domain to frequency domain can be obtained from g(u) by the inverse transformation and form a Fourier transform pair Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_3.htm[6/14/2012 3:53:54 PM] Module 7:Data Representation Lecture 34: DFT and DCT Discrete Fourier Transform (DFT) For discrete case, assume vector x has N components DFT of x, denoted by X, has N components given by Inverse transformation (IDFT) is given by To avoid using separate scaling factors, both can be taken as Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_4.htm[6/14/2012 3:53:54 PM] Module 7:Data Representation Lecture 34: DFT and DCT Properties Parseval's theorem: , i.e., length of vectors is preserved When both scaling factors are Contractive mapping Invertible, linear transformation Essentially, a rotation in N-dimensional space Objectives_template file:///C|/Documents%20and%20Settings/iitkrana1/My%20Documents/Google%20Talk%20Received%20Files/ist_data/lecture34/34_5.htm[6/14/2012 3:53:54 PM] Module 7:Data Representation Lecture 34: DFT and DCT Coefficients Expanding , First coefficient is (scaled) sum or average Other coefficients define the frequency components (cosine and sine) at frequencies forRead More
1. What is the difference between DFT and DCT? | ![]() |
2. How does the DFT work? | ![]() |
3. What are the applications of DCT? | ![]() |
4. How does the DCT differ from the Fourier Transform? | ![]() |
5. What are some limitations of the DFT and DCT? | ![]() |
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