Fourier series. The frequency domain It is sometimes preferable to work in the frequency domain rather than time –Some mathematical operations are easier.

Slides:



Advertisements
Similar presentations
DCSP-11 Jianfeng Feng
Advertisements

Fourier Series 主講者:虞台文.
Fourier Integrals For non-periodic applications (or a specialized Fourier series when the period of the function is infinite: L  ) L -L L  -L  - 
1 Chapter 16 Fourier Analysis with MATLAB Fourier analysis is the process of representing a function in terms of sinusoidal components. It is widely employed.
DFT/FFT and Wavelets ● Additive Synthesis demonstration (wave addition) ● Standard Definitions ● Computing the DFT and FFT ● Sine and cosine wave multiplication.
Fourier Transform – Chapter 13. Image space Cameras (regardless of wave lengths) create images in the spatial domain Pixels represent features (intensity,
Math Review with Matlab:
Signals Processing Second Meeting. Fourier's theorem: Analysis Fourier analysis is the process of analyzing periodic non-sinusoidal waveforms in order.
Fourier Analysis D. Gordon E. Robertson, PhD, FCSB School of Human Kinetics University of Ottawa.
Time and Frequency Representation
Unit 7 Fourier, DFT, and FFT 1. Time and Frequency Representation The most common representation of signals and waveforms is in the time domain Most signal.
Discrete Time Periodic Signals A discrete time signal x[n] is periodic with period N if and only if for all n. Definition: Meaning: a periodic signal keeps.
CH#3 Fourier Series and Transform
Basics of Signal Processing. frequency = 1/T  speed of sound × T, where T is a period sine wave period (frequency) amplitude phase.
Chapter 25 Nonsinusoidal Waveforms. 2 Waveforms Used in electronics except for sinusoidal Any periodic waveform may be expressed as –Sum of a series of.
Where we’re going Speed, Storage Issues Frequency Space.
Basics of Signal Processing. SIGNALSOURCE RECEIVER describe waves in terms of their significant features understand the way the waves originate effect.
Chapter #1: Signals and Amplifiers
Motivation Music as a combination of sounds at different frequencies
Fourier (1) Hany Ferdinando Dept. of Electrical Eng. Petra Christian University.
Fundamentals of Electric Circuits Chapter 17
Chapter 4: Image Enhancement in the Frequency Domain Chapter 4: Image Enhancement in the Frequency Domain.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 Chapter 19.
ME- 495 Mechanical and Thermal Systems Lab Fall 2011 Chapter 4 - THE ANALOG MEASURAND: TIME-DEPENDANT CHARACTERISTICS Professor: Sam Kassegne.
Module 2 SPECTRAL ANALYSIS OF COMMUNICATION SIGNAL.
Wireless and Mobile Computing Transmission Fundamentals Lecture 2.
Chapter 17 The Fourier Series
EE210 Digital Electronics Class Lecture 2 March 20, 2008.
Where we’ve been Attenuate, Amplify, Linearize, Filter.
Why We Use Three Different, Equivalent Forms of the Fourier Series.
Digital Image Processing Chapter 4 Image Enhancement in the Frequency Domain Part I.
1 ELECTRICAL CIRCUIT ET 201  Define and explain phasors, time and phasor domain, phasor diagram.  Analyze circuit by using phasors and complex numbers.
Fundamentals of Electric Circuits Chapter 9
Fourier series: Eigenfunction Approach
By Ya Bao oct 1 Fourier Series Fourier series: how to get the spectrum of a periodic signal. Fourier transform: how.
CT1037N Introduction to Communications Signal Representation & Spectral Analysis Er. Saroj Sharan Regmi Lecture 05.
12/2/2015 Fourier Series - Supplemental Notes A Fourier series is a sum of sine and cosine harmonic functions that approximates a repetitive (periodic)
Fourier Series Fourier Transform Discrete Fourier Transform ISAT 300 Instrumentation and Measurement Spring 2000.
Inverse DFT. Frequency to time domain Sometimes calculations are easier in the frequency domain then later convert the results back to the time domain.
CH#3 Fourier Series and Transform
Vibrationdata 1 Unit 6a The Fourier Transform. Vibrationdata 2 Courtesy of Professor Alan M. Nathan, University of Illinois at Urbana-Champaign.
Sinusoid Seventeenth Meeting. Sine Wave: Amplitude The amplitude is the maximum displacement of the sine wave from its mean (average) position. Simulation.
COMPLEX NUMBERS and PHASORS. OBJECTIVES  Use a phasor to represent a sine wave.  Illustrate phase relationships of waveforms using phasors.  Explain.
The Spectrum n Jean Baptiste Fourier ( ) discovered a fundamental tenet of wave theory.
Lecture 6 (II) COMPLEX NUMBERS and PHASORS. OBJECTIVES A.Use a phasor to represent a sine wave. B.Illustrate phase relationships of waveforms using phasors.
1 EE2003 Circuit Theory Chapter 17 The Fourier Series Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
EEE 332 COMMUNICATION Fourier Series Text book: Louis E. Frenzel. Jr. Principles of Electronic Communication Systems, Third Ed. Mc Graw Hill.
The Frequency Domain Digital Image Processing – Chapter 8.
Chapter 2. Characteristics of Signal ※ Signal : transmission of information The quality of the information depends on proper selection of a measurement.
Frequency Domain Representation of Biomedical Signals.
ELECTRIC CIRCUITS EIGHTH EDITION JAMES W. NILSSON & SUSAN A. RIEDEL.
CH#3 Fourier Series and Transform 1 st semester King Saud University College of Applied studies and Community Service 1301CT By: Nour Alhariqi.
Fourier Analysis Patrice Koehl Department of Biological Sciences National University of Singapore
EE422G Signals and Systems Laboratory Fourier Series and the DFT Kevin D. Donohue Electrical and Computer Engineering University of Kentucky.
Signal Fndamentals Analogue, Discrete and Digital Signals
Introduction to Transforms
COMPLEX NUMBERS and PHASORS
Fourier’s Theorem.
MECH 373 Instrumentation and Measurements
Continuous-Time Signal Analysis
Sinusoidal Waveform Phasor Method.
Periodic Functions and Fourier Series
Net 222: Communications and networks fundamentals (Practical Part)
Fourier Integrals For non-periodic applications (or a specialized Fourier series when the period of the function is infinite: L) -L L -L- L
Image Processing, Leture #14
I. Previously on IET.
EE210 Digital Electronics Class Lecture 2 September 03, 2008
Engineering Circuit Analysis
Discrete Fourier Transform
The Frequency Domain Any wave shape can be approximated by a sum of periodic (such as sine and cosine) functions. a--amplitude of waveform f-- frequency.
Presentation transcript:

Fourier series

The frequency domain It is sometimes preferable to work in the frequency domain rather than time –Some mathematical operations are easier in the frequency domain –the human ear works on frequencies Working in this domain really means the x axis is f and not t. We need a method to convert time domain functions into frequency domain functions

Fourier Series A sinusoid can be represented by A sinusoid can be expressed as a sum of a sine and cosine at the same frequency but possibly different magnitudes independently of phase

Adding sinusoids with freq F results in a sinusoid with frequency F x(t)=sin(4πt) + 0.6cos(4πt)

Any periodic waveform can be represented as an infinite sum of sine and cosine waves regardless of phase (as shown in the previous slide). This is the Fourier Series f(t) Or more succinctly written as: a 0 =const, a n and b n are the amplitudes of the individual harmonics making up the periodic waveform

Discrete Fourier Transform DFT The data we will use is sampled and an infinite number of samples is impractical Works with non continuous non periodic functions N time domain samples transform to N complex DFT values in the frequency domain

Periodic function generation Remember that you created a sine wave digitally using:

The DFT is: Where F is effectively a row matrix of size N h is the harmonic n is the time domain sample number x(n) is the magnitude of the n th sample N is the total number of samples

As each Fourier coefficient F(h) is complex so its magnitude and phase (with respect to the fundamental) need to be calculated:

Example Consider 4 samples of a waveform from the time domain (from an a to d converter) {1,0,0,1}

Show that x(2)=0 and x(3)=1-j So the DFT of a time vector {1,0,0,1} is a vector {2,1+j,0,1-j} These coefficients are frequency independent as no account for frequency has been taken. We know that the second coefficient F(1) will represent the fundamental and the next one F(2) will be the next harmonic etc. If we need to find the fundamental frequency, we need to specify the coefficient in terms of sample frequency F s where

Power phase diagram Often wish to represent Fourier spectrum diagrammatically Power is magnitude squared Phase is angle Line up power graph with phase graph Plot actual frequencies is sample rate known Usually only plot samples from 0 to N/2

From example x = {1,0,0,1} giving Fourier coefficients of {2,1+j,0,1-j} If F s =1000Hz, F 1 =1000/N=250, F 2 =500, F 3 =750 Polar form of power and phase:

90 45 F M k