1 / 107

Chapter 8 The Discrete Fourier Transform

Chapter 8 The Discrete Fourier Transform. Biomedical Signal processing. Zhongguo Liu Biomedical Engineering School of Control Science and Engineering, Shandong University. 1. Chapter 8 The Discrete Fourier Transform. 8.0 Introduction

ardara
Télécharger la présentation

Chapter 8 The Discrete Fourier Transform

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Chapter 8 The Discrete Fourier Transform Biomedical Signal processing Zhongguo Liu Biomedical Engineering School of Control Science and Engineering, Shandong University 1 Zhongguo Liu_Biomedical Engineering_Shandong Univ.

  2. Chapter 8 The Discrete Fourier Transform • 8.0 Introduction • 8.1 Representation of Periodic Sequence: the Discrete Fourier Series • 8.2 Properties of the Discrete Fourier Series • 8.3 The Fourier Transform of Periodic Signal • 8.4 Sampling the Fourier Transform • 8.5 Fourier Representation of Finite-Duration Sequence: the Discrete Fourier Transform • 8.6 Properties of the Discrete Fourier Transform • 8.7 Linear Convolution using the Discrete Fourier Transform

  3. Filter Design Techniques 8.0 Introduction

  4. 8.0 Introduction • Discrete Fourier Transform (DFT)for finite duration sequence • DFT is a sequence rather than a function of a continuous variable • DFT corresponds to sample, equally spaced in frequency, of the Fourier transform of the signal.

  5. 8.0 Introduction • The relationship between periodic sequence and finite-length sequences: • The Fourier series representation of the periodic sequence corresponds to the DFT of the finite-length sequence.

  6. Given a periodic sequence with period N so that 8.1 Representation of Periodic Sequence: the Discrete Fourier Series • The Fourier series representation can be written as • Fourier series representation of continuous-time periodic signals require infinite many complex exponentials • Not that for discrete-time periodic signals we have

  7. 8.1 Representation of Periodic Sequence: the Discrete Fourier Series • Due to the periodicity of the complex exponential we only need N exponentials for discrete time Fourier series • No need

  8. To obtain the Fourier series coefficients we multiply both sides by for 0nN-1 and then sum both the sides , we obtain Discrete Fourier Series Pair • A periodic sequence in terms of Fourier series coefficients

  9. Discrete Fourier Series Pair Problem 8.51, HW

  10. The Fourier series coefficients of is 8.1 Representation of Periodic Sequence: the Discrete Fourier Series • a periodic sequence with period N,

  11. The sequence is periodic with period N 8.1 Representation of Periodic Sequence: the Discrete Fourier Series

  12. Synthesis equation: Discrete Fourier Series (DFS) • Let • Analysis equation:

  13. N points …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 Ex. 8.1 DFS of a impulse train • Consider the periodic impulse train n

  14. N points k …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 Ex. 8.1 DFS of a impulse train

  15. N points 1 k …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 N points 1 n …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1

  16. - N 1 ~ N points [ ] [ ] ~ å = kn X k x n W N N = n 0 …… …… …… -N N 1 2 -2 -1 0 Example 8.2 Duality in the Discrete Fourier Series • The discrete Fourier series coefficients is the periodic impulse train

  17. N points N …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 N points 1 …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 k n

  18. N points 1 k …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 N points N N points …… …… 1 …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 N points 1 n …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1 …… …… …… 2 N-1 N N+1 N+2 -N -N+1 -2 -1 0 1

  19. Example 8.3 The Discrete Fourier Series of a Periodic Rectangular Pulse Train • Periodic sequence with period N=10 1

  20. magnitude phase

  21. magnitude phase

  22. 8.2 Properties of the Discrete Fourier Series • Linearity: two periodic sequence, both with period N

  23. 8.2 Properties of the Discrete Fourier Series • Shift of a sequence Problem 8.52, HW

  24. N k …… 2 N-1 0 1 1 1 n 1 …… 2 N-1 0 1 k …… N-1 2 0 1 n …… 2 N-1 0 1 8.2 Properties of the Discrete Fourier Series • Duality

  25. 8.2.4 Symmetry Problem 8.53, HW

  26. and are two periodic sequences, each with period N and with discrete Fourier series and 8.2.5 Periodic Convolution

  27. The sum is over the finite interval • The value of in the interval repeat periodically for m outside of that interval 8.2.5 Periodic Convolution

  28. Example 8.4 Periodic Convolution

  29. 8.2.5 Periodic Convolution

  30. The Fourier series coefficients of is 8.1 Representation of Periodic Sequence: the Discrete Fourier Series • a periodic sequence with period N, Review

  31. Synthesis equation: Discrete Fourier Series (DFS) • Let • Analysis equation:

  32. 8.2 Properties of the Discrete Fourier Series • Shift of a sequence

  33. N k …… 2 N-1 0 1 1 1 n 1 …… 2 N-1 0 1 k …… N-1 2 0 1 n …… 2 N-1 0 1 8.2 Properties of the Discrete Fourier Series • Duality

  34. 8.2.5 Periodic Convolution

  35. Example 8.4 Periodic Convolution

  36. 8.3 The Fourier Transform of Periodic Signal • Periodic sequences are neither absolutely summable nor square summable, hence they don’t have a strict Fourier Transform

  37. 8.3 The Fourier Transform of Periodic Signal • We can represent Periodic sequences as sums of complex exponentials: DFS • We can combine DFS and Fourier transform • Fourier transform of periodic sequences • Periodic impulse train with values proportional to DFS coefficients

  38. 8.3 The Fourier Transform of Periodic Signal This is periodic with 2 since DFS is periodic • The inverse transform can be written as

  39. N points 1 • The DFS was calculated previously to be …… …… …… N points -N N 1 2 -2 -1 0 1 …… …… …… n 2 N-1 N -N -2 -1 0 1 • Therefore the Fourier transform is Ex. 8.5 Fourier Transform of a periodic impulse train • Consider the periodic impulse train

  40. 1 …… …… -N N 1 2 -2 -1 0 Relation between Finite-length and Periodic Signals • Consider finite length signal x[n] spanning from 0 to N-1 • Convolve with periodic impulse train • The Fourier transform of the periodic sequence is

  41. Relation between Finite-length and Periodic Signals • This implies that • DFS coefficients of a periodic signal can be thought as equally spaced samples of the Fourier transform of one period

  42. If is periodic with period N, the DFS are • If for and otherwise Relation between Finite-length and Periodic Signals then

  43. Ex. 8.5 Relation between FS coefficients and FT • Consider the sequence • The Fourier transform

  44. Ex. 8.5 Relation between FS coefficients and FT • The Fourier transform • The DFS coefficients • Consider the sequence

  45. The Fourier transform • The DFS coefficients Ex. 8.5 Relation between FS coefficients and FT • Consider the sequence

  46. Consider an aperiodic sequence with Fourier transform ,and assume that a sequence is obtained by sampling at frequency • is Fourier series coefficients of periodic sequence 8.4 Sampling the Fourier Transform

  47. Sampling the Fourier Transform

  48. N points 1 …… …… …… -N N 1 2 -2 -1 0 Sampling the Fourier Transform

  49. Sampling the Fourier Transform

  50. Sampling the Fourier Transform • Samples of the DTFT of an aperiodic sequence • can be thought of as DFS coefficients • of a periodic sequence • obtained through summing periodic replicas of original sequence • If the original sequence is of finite length, • and we take sufficient number of samples of its DTFT, • then the original sequence can be recovered by

More Related