Lecture 24: CT Fourier Transform

Slides:



Advertisements
Similar presentations
Signal Processing in the Discrete Time Domain Microprocessor Applications (MEE4033) Sogang University Department of Mechanical Engineering.
Advertisements

ECE 8443 – Pattern Recognition EE 3512 – Signals: Continuous and Discrete Objectives: Response to a Sinusoidal Input Frequency Analysis of an RC Circuit.
Lecture 7: Basis Functions & Fourier Series
Leo Lam © Signals and Systems EE235. Transformers Leo Lam ©
Signals and Systems – Chapter 5
SIGNAL AND SYSTEM CT Fourier Transform. Fourier’s Derivation of the CT Fourier Transform x(t) -an aperiodic signal -view it as the limit of a periodic.
EE-2027 SaS 06-07, L11 1/12 Lecture 11: Fourier Transform Properties and Examples 3. Basis functions (3 lectures): Concept of basis function. Fourier series.
Lecture 19: Discrete-Time Transfer Functions
EE-2027 SaS, L15 1/15 Lecture 15: Continuous-Time Transfer Functions 6 Transfer Function of Continuous-Time Systems (3 lectures): Transfer function, frequency.
PROPERTIES OF FOURIER REPRESENTATIONS
Lecture 14: Laplace Transform Properties
APPLICATIONS OF FOURIER REPRESENTATIONS TO
^ y(t) Model u(t) u(t) y(t) Controller Plant h(t), H(jw)
EE-2027 SaS, L11 1/13 Lecture 11: Discrete Fourier Transform 4 Sampling Discrete-time systems (2 lectures): Sampling theorem, discrete Fourier transform.
Lecture 9: Fourier Transform Properties and Examples
Leo Lam © Signals and Systems EE235. Leo Lam © Fourier Transform Q: What did the Fourier transform of the arbitrary signal say to.
Leo Lam © Signals and Systems EE235 Lecture 27.
Chapter 4 The Fourier Transform EE 207 Dr. Adil Balghonaim.
Leo Lam © Signals and Systems EE235 Lecture 31.
Leo Lam © Signals and Systems EE235. Leo Lam © x squared equals 9 x squared plus 1 equals y Find value of y.
Leo Lam © Signals and Systems EE235. Leo Lam © Fourier Transform Q: What did the Fourier transform of the arbitrary signal say to.
The sampling of continuous-time signals is an important topic It is required by many important technologies such as: Digital Communication Systems ( Wireless.
Prof. Nizamettin AYDIN Digital Signal Processing 1.
Single-Sideband AM A DSB-SC AM signal transmits two sidebands and required a channel bandwidth of Bc = 2W Hz However, the two sidebands are redundant The.
ECE 8443 – Pattern Recognition EE 3512 – Signals: Continuous and Discrete Objectives: Linearity Time Shift and Time Reversal Multiplication Integration.
Digital Signal Processing
CISE315 SaS, L171/16 Lecture 8: Basis Functions & Fourier Series 3. Basis functions: Concept of basis function. Fourier series representation of time functions.
1 Review of Continuous-Time Fourier Series. 2 Example 3.5 T/2 T1T1 -T/2 -T 1 This periodic signal x(t) repeats every T seconds. x(t)=1, for |t|
Signal and Systems Prof. H. Sameti Chapter 5: The Discrete Time Fourier Transform Examples of the DT Fourier Transform Properties of the DT Fourier Transform.
Fourier Series. Introduction Decompose a periodic input signal into primitive periodic components. A periodic sequence T2T3T t f(t)f(t)
Chapter 5 Z Transform. 2/45  Z transform –Representation, analysis, and design of discrete signal –Similar to Laplace transform –Conversion of digital.
Fundamentals of Electric Circuits Chapter 18 Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display.
Chapter 4 Fourier transform Prepared by Dr. Taha MAhdy.
Course Outline (Tentative) Fundamental Concepts of Signals and Systems Signals Systems Linear Time-Invariant (LTI) Systems Convolution integral and sum.
Linearity Recall our expressions for the Fourier Transform and its inverse: The property of linearity: Proof: (synthesis) (analysis)
Lecture 17: The Discrete Fourier Series Instructor: Dr. Ghazi Al Sukkar Dept. of Electrical Engineering The University of Jordan
Input Function x(t) Output Function y(t) T[ ]. Consider The following Input/Output relations.
Signals and Systems Prof. H. Sameti Chapter 4: The Continuous Time Fourier Transform Derivation of the CT Fourier Transform pair Examples of Fourier Transforms.
ES97H Biomedical Signal Processing
Chapter 7 The Laplace Transform
EE 207 Dr. Adil Balghonaim Chapter 4 The Fourier Transform.
Fourier Representation of Signals and LTI Systems.
ABE 463 Electro-hydraulic systems Laplace transform Tony Grift
Min-Plus Linear Systems Theory Min-Plus Linear Systems Theory.
Signals and Systems Lecture #6 EE3010_Lecture6Al-Dhaifallah_Term3321.
1 Fourier Representation of Signals and LTI Systems. CHAPTER 3 UniMAP.
Oh-Jin Kwon, EE dept., Sejong Univ., Seoul, Korea: 2.3 Fourier Transform: From Fourier Series to Fourier Transforms.
Leo Lam © Signals and Systems EE235 Lecture 25.
بسم الله الرحمن الرحيم University of Khartoum Department of Electrical and Electronic Engineering Third Year – 2015 Dr. Iman AbuelMaaly Abdelrahman
ENEE 322: Continuous-Time Fourier Transform (Chapter 4)
Leo Lam © Signals and Systems EE235 Lecture 26.
Math for CS Fourier Transforms
Lecture 7: Basis Functions & Fourier Series
CHAPTER 5 Z-Transform. EKT 230.
CE Digital Signal Processing Fall Discrete-time Fourier Transform
LECTURE 11: FOURIER TRANSFORM PROPERTIES
Laplace and Z transforms
Signals and Systems EE235 Lecture 26 Leo Lam ©
Chapter 15 Introduction to the Laplace Transform
UNIT II Analysis of Continuous Time signal
The sampling of continuous-time signals is an important topic
Signals and Systems EE235 Lecture 31 Leo Lam ©
Chapter 3 Convolution Representation
Fundamentals of Electric Circuits Chapter 18
Fundamentals of Electric Circuits Chapter 15
LECTURE 18: FOURIER ANALYSIS OF CT SYSTEMS
Signals & Systems (CNET - 221) Chapter-5 Fourier Transform
4. The Continuous time Fourier Transform
LECTURE 11: FOURIER TRANSFORM PROPERTIES
SIGNALS & SYSTEMS (ENT 281)
Presentation transcript:

Lecture 24: CT Fourier Transform CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L24

CISE315, L27

CISE315, L27

CISE315, L27

CISE315, L27

CISE315, L27

Symmetry Property: Example CISE315, L27

CISE315, L27

Property of Duality CISE315, L27

Illustration of the duality property CISE315, L27

More Properties CISE315, L27

Example: Fourier Transform of a Step Signal Lets calculate the Fourier transform X(jw)of x(t) = u(t), making use of the knowledge that: and noting that: Taking Fourier transform of both sides using the integration property. Since G(jw) = 1: We can also apply the differentiation property in reverse CISE315, L27

Convolution Property CISE315, L27

Proof of Convolution Property Taking Fourier transforms gives: Interchanging the order of integration, we have By the time shift property, the bracketed term is e-jwtH(jw), so CISE315, L27

Convolution in the Frequency Domain To solve for the differential/convolution equation using Fourier transforms: Calculate Fourier transforms of x(t) and h(t) Multiply H(jw) by X(jw) to obtain Y(jw) Calculate the inverse Fourier transform of Y(jw) Multiplication in the frequency domain corresponds to convolution in the time domain and vice versa. CISE315, L27

Example 1: Solving an ODE Consider the LTI system time impulse response to the input signal Transforming these signals into the frequency domain and the frequency response is to convert this to the time domain, express as partial fractions: Therefore, the time domain response is: ba CISE315, L27

Example 2: Designing a Low Pass Filter H(jw) wc -wc Lets design a low pass filter: The impulse response of this filter is the inverse Fourier transform which is an ideal low pass filter Non-causal (how to build) The time-domain oscillations may be undesirable How to approximate the frequency selection characteristics? Consider the system with impulse response: Causal and non-oscillatory time domain response and performs a degree of low pass filtering CISE315, L27

Modulation property CISE315, L27

Lecture 27: Summary The Fourier transform is widely used for designing filters. You can design systems which reject high frequency noise and just retain the low frequency components. This is natural to describe in the frequency domain. Important properties of the Fourier transform are: 1. Linearity and time shifts 2. Differentiation 3. Convolution Some operations are simplified in the frequency domain, but there are a number of signals for which the Fourier transform do not exist – this leads naturally onto Laplace transforms CISE315, L27