3F4 Power and Energy Spectral Density Dr. I. J. Wassell.

Slides:



Advertisements
Similar presentations
Definitions Periodic Function: f(t +T) = f(t)t, (Period T)(1) Ex: f(t) = A sin(2Πωt + )(2) has period T = (1/ω) and ω is said to be the frequency (angular),
Advertisements

3F4 Line Coding Dr. I. J. Wassell. Introduction Line coding is the procedure used to convert an incoming bit stream, b k to symbols a k which are then.
Ch 3 Analysis and Transmission of Signals
1 / 13 Fourier, bandwidth, filter. 2 / 13 The important roles of Fourier series and Fourier transforms: –To analysis and synthesis signals in frequency.
Sampling process Sampling is the process of converting continuous time, continuous amplitude analog signal into discrete time continuous amplitude signal.
ELEC 303 – Random Signals Lecture 20 – Random processes
Noise. Noise is like a weed. Just as a weed is a plant where you do not wish it to be, noise is a signal where you do not wish it to be. The noise signal.
Lecture 6 Power spectral density (PSD)
EE322 Digital Communications
Sep 22, 2005CS477: Analog and Digital Communications1 Random Processes and PSD Analog and Digital Communications Autumn
3F4 Optimal Transmit and Receive Filtering Dr. I. J. Wassell.
Review of Probability and Random Processes
FOURIER TRANSFORMS.
Matched Filters By: Andy Wang.
Analogue and digital techniques in closed loop regulation applications Digital systems Sampling of analogue signals Sample-and-hold Parseval’s theorem.
Sep 20, 2005CS477: Analog and Digital Communications1 Random variables, Random processes Analog and Digital Communications Autumn
1 For a deterministic signal x(t), the spectrum is well defined: If represents its Fourier transform, i.e., if then represents its energy spectrum. This.
Digital Communication
ELEC 303 – Random Signals Lecture 21 – Random processes
Formatting and Baseband Modulation
ELEC ENG 4035 Communications IV1 School of Electrical & Electronic Engineering 1 Section 2: Frequency Domain Analysis Contents 2.1 Fourier Series 2.2 Fourier.
Random Process The concept of random variable was defined previously as mapping from the Sample Space S to the real line as shown below.
Lecture 1. References In no particular order Modern Digital and Analog Communication Systems, B. P. Lathi, 3 rd edition, 1998 Communication Systems Engineering,
1 Let g(t) be periodic; period = T o. Fundamental frequency = f o = 1/ T o Hz or  o = 2  / T o rad/sec. Harmonics =n f o, n =2,3 4,... Trigonometric.
EBB Chapter 2 SIGNALS AND SPECTRA Chapter Objectives: Basic signal properties (DC, RMS, dBm, and power); Fourier transform and spectra; Linear systems.
6.2 - The power Spectrum of a Digital PAM Signal A digtal PAM signal at the input to a communication channl scale factor (where 2d is the “Euclidean.
TELECOMMUNICATIONS Dr. Hugh Blanton ENTC 4307/ENTC 5307.
Random Processes ECE460 Spring, Power Spectral Density Generalities : Example: 2.
1 Part 5 Response of Linear Systems 6.Linear Filtering of a Random Signals 7.Power Spectrum Analysis 8.Linear Estimation and Prediction Filters 9.Mean-Square.
ECE 8443 – Pattern Recognition ECE 3163 – Signals and Systems Objectives: The Trigonometric Fourier Series Pulse Train Example Symmetry (Even and Odd Functions)
EE313 Linear Systems and Signals Fall 2010 Initial conversion of content to PowerPoint by Dr. Wade C. Schwartzkopf Prof. Brian L. Evans Dept. of Electrical.
Vibrationdata 1 Unit 9 White Noise FFT. Vibrationdata 2 Fourier Transform, Sine Function A Fourier transform will give the exact magnitude and frequency.
Spread Spectrum Modulation Dr. Teerasit Kasetkasem.
EE104: Lecture 5 Outline Review of Last Lecture Introduction to Fourier Transforms Fourier Transform from Fourier Series Fourier Transform Pair and Signal.
Chapter 2 Signals and Spectra (All sections, except Section 8, are covered.)
Fourier Analysis of Signals and Systems
Random Processes and Spectral Analysis
revision Transfer function. Frequency Response
Chapter 1 Random Process
Dept. of EE, NDHU 1 Chapter One Signals and Spectra.
EE 495 Modern Navigation Systems Noise & Random Processes Mon, March 02 EE 495 Modern Navigation Systems Slide 1 of 19.
The Trigonometric Fourier Series Representations
Chapter 2. Fourier Representation of Signals and Systems
Geology 6600/7600 Signal Analysis 21 Sep 2015 © A.R. Lowry 2015 Last time: The Cross-Power Spectrum relating two random processes x and y is given by:
Discrete-time Random Signals
Geology 6600/7600 Signal Analysis 28 Sep 2015 © A.R. Lowry 2015 Last time: Energy Spectral Density; Linear Systems given (deterministic) finite-energy.
1 Review of Probability and Random Processes. 2 Importance of Random Processes Random variables and processes talk about quantities and signals which.
EEE Chapter 6 Random Processes and LTI Huseyin Bilgekul EEE 461 Communication Systems II Department of Electrical and Electronic Engineering Eastern.
Oh-Jin Kwon, EE dept., Sejong Univ., Seoul, Korea: 2.3 Fourier Transform: From Fourier Series to Fourier Transforms.
The Trigonometric Fourier Series Representations
Random process UNIT III Prepared by: D.MENAKA, Assistant Professor, Dept. of ECE, Sri Venkateswara College of Engineering, Sriperumbudur, Tamilnadu.
Digital Communications Chapter 1 Signals and Spectra Signal Processing Lab.
Eeng360 1 Chapter 2 Linear Systems Topics:  Review of Linear Systems Linear Time-Invariant Systems Impulse Response Transfer Functions Distortionless.
ELECTRIC CIRCUITS EIGHTH EDITION JAMES W. NILSSON & SUSAN A. RIEDEL.
Fourier Transform and Spectra
Chapter 6 Random Processes
 Carrier signal is strong and stable sinusoidal signal x(t) = A cos(  c t +  )  Carrier transports information (audio, video, text, ) across.
Properties of the power spectral density (1/4)
UNIT-III Signal Transmission through Linear Systems
SIGNALS PROCESSING AND ANALYSIS
Outline Introduction Signal, random variable, random process and spectra Analog modulation Analog to digital conversion Digital transmission through baseband.
Laboratory in Oceanography: Data and Methods
Random Process The concept of random variable was defined previously as mapping from the Sample Space S to the real line as shown below.
Chapter 2 Linear Systems
The Fourier Series for Continuous-Time Periodic Signals
8.6 Autocorrelation instrument, mathematical definition, and properties autocorrelation and Fourier transforms cosine and sine waves sum of cosines Johnson.
For a deterministic signal x(t), the spectrum is well defined: If
Chapter 2 SIGNALS AND SPECTRA Chapter Objectives:
Fourier Transform and Spectra
copyright Robert J. Marks II
Presentation transcript:

3F4 Power and Energy Spectral Density Dr. I. J. Wassell

Power and Energy Spectral Density The power spectral density (PSD) S x (  ) for a signal is a measure of its power distribution as a function of frequency It is a useful concept which allows us to determine the bandwidth required of a transmission system We will now present some basic results which will be employed later on

PSD Consider a signal x(t) with Fourier Transform (FT) X(  ) We wish to find the energy and power distribution of x(t) as a function of frequency

Deterministic Signals If x(t) is the voltage across a R=1  resistor, the instantaneous power is, Thus the total energy in x(t) is, From Parseval’s Theorem,

Deterministic Signals So, Where E(2  f) is termed the Energy Density Spectrum (EDS), since the energy of x(t) in the range f o to f o +  f o is,

Deterministic Signals For communications signals, the energy is effectively infinite (the signals are of unlimited duration), so we usually work with Power quantities We find the average power by averaging over time Where x T (t) is the same as x(t), but truncated to zero outside the time window -T/2 to T/2 Using Parseval as before we obtain,

Deterministic Signals Where S x (  ) is the Power Spectral Density (PSD)

PSD The power dissipated in the range f o to f o +  f o is, And S x (.) has units Watts/Hz

Wiener-Khintchine Theorem It can be shown that the PSD is also given by the FT of the autocorrelation function (ACF), r xx (  ), Where,

Random Signals The previous results apply to deterministic signals In general, we deal with random signals, eg the transmitted PAM signal is random because the symbols (a k ) take values at random Fortunately, our earlier results can be extended to cover random signals by the inclusion of an extra averaging or expectation step, over all possible values of the random signal x(t)

PSD, random signals The W-K result holds for random signals, choosing for x(t) any randomly selected realisation of the signal Where E[.] is the expectation operator Note: Only applies for ergodic signals where the time averages are the same as the corresponding ensemble averages

Linear Systems and Power Spectra Passing x T (t) through a linear filter H(  ) gives the output spectrum, Hence, the output PSD is,