Fourier Transform. louder softer. louder. softer. amplitude. time. amplitude. time. frequency. frequency. P. J. Grandinetti
|
|
- Rosanna Jones
- 5 years ago
- Views:
Transcription
1 Fourier Transform * * amplitude louder softer amplitude louder softer frequency frequency
2 Fourier Transform amplitude What is the mathematical relationship between two signal domains frequency
3 Fourier Transform amplitude frequency
4 Inverse Fourier Transform amplitude frequency
5 Simple Fourier Transform Example
6 Simple Fourier Transform Example
7 Simple Fourier Transform Example FT
8 Simple Fourier Transform Example FT Ω 0 Ω frequency
9 Simple Fourier Transform Example FT Ω 0 What is the meaning of negative frequency? Ω frequency
10 Circular (Counter Clockwise) Motion in Complex Plane y r x -r r x r y -r FT Ω 0 Ω frequency
11 Circular (Clockwise) Motion in Complex Plane y r x -r r x r y -r FT Ω 0 Ω frequency
12 Exponential Decay : Lorentzian Lineshape X Y Lorentzian
13 Exponential Decay : Lorentzian Lineshape FT Ω Ω Real Imaginary Absorption Mode 2/T 2 Dispersion Mode 2/T 2
14 In a perfect world... Spectral Phase Correction path of tip of magnetization vector as it precesses x detector y detector Real Imaginary
15 Spectral Phase Correction : Zeroth Order First problem is a minor one... φ Receiver phase of zero does not correspond to zero phase from x in rotating frame. Depends on cable lengths and probe tuning. Otherwise should remain constant. x detector y detector Real Imaginary Absorption and Dispersion mode lineshapes become mixed in real and imaginary parts.
16 Spectral Phase Correction : Zeroth Order Solution is simple... Real Imaginary Absorption and Dispersion mode lineshapes mixed in real and imaginary parts. Real Imaginary Absorption and Dispersion mode lineshapes cleanly separated into real and imaginary parts.
17 Spectral Phase Correction : First Order Ω 2 Ω 1 X Real Imaginary Ω 1 Ω 2 y at t=0, when receiver is turned on, the two magnetization vectors are aligned along x axis.
18 Spectral Phase Correction : First Order Ω 2 Ω 1 X Real Imaginary Ω 1 Ω 2 y at t=0, when receiver is turned on, the two magnetization vectors are aligned along x axis. What happens if we were late in turning on the receiver?
19 Spectral Phase Correction : First Order Receiver is turn on at t 0 after pulse. Ω 1 Ω 1 X Real Ω 2 Imaginary Ω 2 y Phase needed to make site 1 have a pure absorption mode spectrum in real part is not the same as the phase needed for site 2. The phase correction needed can be calculated from the frequency of each site. We define phase correction as linearly dependent on frequency: that we were late in starting the detector
20 Spectral Phase Correction : First Order Ω 1 Real Ω 2 Imaginary Ω 1 Ω 2 Real Imaginary
21 Spectral Phase Correction : First Order Ω 1 Real Ω 2 Imaginary Ω 1 Ω 2 Real Imaginary Somes see baseline roll
22 Spectral Phase Correction : First Order S 1 (t) F. T. S 1 (ν) S 2 (t) 1 0 X = (Multiplication) F. T. S 2 (ν) * = (Convolution) S T (t) F. T. S T (ν)
23 Spectral Phase Correction : Algorithm ν
24 Spectral Phase Correction : Algorithm ν Ω 1 Apply zeroth order phase correction until one peak is completely absorption mode lineshape. one peak "phased" ν
25 Spectral Phase Correction : Algorithm ν No further phase correction should affect this peak Ω 1 Apply zeroth order phase correction until one peak is completely absorption mode lineshape. one peak "phased" ν
26 Spectral Phase Correction : Algorithm ν No further phase correction should affect this peak Ω 1 Apply zeroth order phase correction until one peak is completely absorption mode lineshape. one peak "phased" ν Pivot Frequency
27 Spectral Phase Correction : Algorithm ν No further phase correction should affect this peak Ω 1 Apply zeroth order phase correction until one peak is completely absorption mode lineshape. one peak "phased" ν Pivot Frequency Adjust t 0 until spectrum is phased. ν
NMR Basics. Lecture 2
NMR Basics Lecture 2 Continuous wave (CW) vs. FT NMR There are two ways of tuning a piano: - key by key and recording each sound (or frequency). - or, kind of brutal, is to hit with a sledgehammer and
More informationLecture 3 Complex Exponential Signals
Lecture 3 Complex Exponential Signals Fundamentals of Digital Signal Processing Spring, 2012 Wei-Ta Chu 2012/3/1 1 Review of Complex Numbers Using Euler s famous formula for the complex exponential The
More informationRF pulse design and the Small Tip Angle Approximation
RF pulse design and the Small Tip Angle Approximation Dr Shaihan J Malik Lecturer in Imaging Sciences Division of Imaging Sciences & Biomedical Engineering King s College London shaihan.malik@kcl.ac.uk
More informationSignals A Preliminary Discussion EE442 Analog & Digital Communication Systems Lecture 2
Signals A Preliminary Discussion EE442 Analog & Digital Communication Systems Lecture 2 The Fourier transform of single pulse is the sinc function. EE 442 Signal Preliminaries 1 Communication Systems and
More informationMAGNETIC RESONANCE IMAGING
CSEE 4620 Homework 3 Fall 2018 MAGNETIC RESONANCE IMAGING 1. THE PRIMARY MAGNET Magnetic resonance imaging requires a very strong static magnetic field to align the nuclei. Modern MRI scanners require
More informationExam Signal Detection and Noise
Exam Signal Detection and Noise Tuesday 27 January 2015 from 14:00 until 17:00 Lecturer: Sense Jan van der Molen Important: It is not allowed to use a calculator. Complete each question on a separate piece
More informationPolarization Experiments Using Jones Calculus
Polarization Experiments Using Jones Calculus Reference http://chaos.swarthmore.edu/courses/physics50_2008/p50_optics/04_polariz_matrices.pdf Theory In Jones calculus, the polarization state of light is
More informationAn induced emf is the negative of a changing magnetic field. Similarly, a self-induced emf would be found by
This is a study guide for Exam 4. You are expected to understand and be able to answer mathematical questions on the following topics. Chapter 32 Self-Induction and Induction While a battery creates an
More informationIntroduction to Wavelet Transform. Chapter 7 Instructor: Hossein Pourghassem
Introduction to Wavelet Transform Chapter 7 Instructor: Hossein Pourghassem Introduction Most of the signals in practice, are TIME-DOMAIN signals in their raw format. It means that measured signal is a
More informationCSC475 Music Information Retrieval
CSC475 Music Information Retrieval Sinusoids and DSP notation George Tzanetakis University of Victoria 2014 G. Tzanetakis 1 / 38 Table of Contents I 1 Time and Frequency 2 Sinusoids and Phasors G. Tzanetakis
More informationSAMPLING THEORY. Representing continuous signals with discrete numbers
SAMPLING THEORY Representing continuous signals with discrete numbers Roger B. Dannenberg Professor of Computer Science, Art, and Music Carnegie Mellon University ICM Week 3 Copyright 2002-2013 by Roger
More informationSHF Communication Technologies AG
SHF Communication Technologies AG Wilhelm-von-Siemens-Str. 23 Aufgang D 2277 Berlin Marienfelde Germany Phone ++49 30 / 772 05 0 Fax ++49 30 / 753 0 78 E-Mail: sales@shf.biz Web: http://www.shf.biz Tutorial
More information10. Phase Cycling and Pulsed Field Gradients Introduction to Phase Cycling - Quadrature images
10. Phase Cycling and Pulsed Field Gradients 10.1 Introduction to Phase Cycling - Quadrature images The selection of coherence transfer pathways (CTP) by phase cycling or PFGs is the tool that allows the
More informationPULSED NUCLEAR MAGNETIC RESONANCE. Advanced Laboratory, Physics 407 University of Wisconsin Madison, Wisconsin 53706
(revised, 2/12/07) PULSED NUCLEAR MAGNETIC RESONANCE Advanced Laboratory, Physics 407 University of Wisconsin Madison, Wisconsin 53706 Abstract A pulsed nuclear magnetic resonance technique (spin-echo)
More informationMETR 3223, Physical Meteorology II: Radar Doppler Velocity Estimation
METR 3223, Physical Meteorology II: Radar Doppler Velocity Estimation Mark Askelson Adapted from: Doviak and Zrnić, 1993: Doppler radar and weather observations. 2nd Ed. Academic Press, 562 pp. I. Essentials--Wave
More informationz t h l g 2009 John Wiley & Sons, Inc. Published 2009 by John Wiley & Sons, Inc.
x w z t h l g Figure 10.1 Photoconductive switch in microstrip transmission-line geometry: (a) top view; (b) side view. Adapted from [579]. Copyright 1983, IEEE. I g G t C g V g V i V r t x u V t Z 0 Z
More informationPrinciples of Planar Near-Field Antenna Measurements. Stuart Gregson, John McCormick and Clive Parini. The Institution of Engineering and Technology
Principles of Planar Near-Field Antenna Measurements Stuart Gregson, John McCormick and Clive Parini The Institution of Engineering and Technology Contents Preface xi 1 Introduction 1 1.1 The phenomena
More informationBackground (~EE369B)
Background (~EE369B) Magnetic Resonance Imaging D. Nishimura Overview of NMR Hardware Image formation and k-space Excitation k-space Signals and contrast Signal-to-Noise Ratio (SNR) Pulse Sequences 13
More informationEfficacy of Wavelet Transform Techniques for. Denoising Polarized Target NMR Signals
Efficacy of Wavelet Transform Techniques for Denoising Polarized Target NMR Signals James Maxwell May 2, 24 Abstract Under the guidance of Dr. Donal Day, mathematical techniques known as Wavelet Transforms
More informationH Micro-Imaging. Tuning and Matching. i. Open any 1H data set and type wobb.
- 1-1 H Micro-Imaging The NMR-specific properties of the objects are visualized as multidimensional images. Translational motion can be observed and spectroscopic information can be spatially resolved.
More information레이저의주파수안정화방법및그응용 박상언 ( 한국표준과학연구원, 길이시간센터 )
레이저의주파수안정화방법및그응용 박상언 ( 한국표준과학연구원, 길이시간센터 ) Contents Frequency references Frequency locking methods Basic principle of loop filter Example of lock box circuits Quantifying frequency stability Applications
More informationSinusoids and Phasors (Chapter 9 - Lecture #1) Dr. Shahrel A. Suandi Room 2.20, PPKEE
Sinusoids and Phasors (Chapter 9 - Lecture #1) Dr. Shahrel A. Suandi Room 2.20, PPKEE Email:shahrel@eng.usm.my 1 Outline of Chapter 9 Introduction Sinusoids Phasors Phasor Relationships for Circuit Elements
More informationAcoustics and Fourier Transform Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018
1 Acoustics and Fourier Transform Physics 3600 - Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018 I. INTRODUCTION Time is fundamental in our everyday life in the 4-dimensional
More informationSpectral Line Imaging
ATNF Synthesis School 2003 Spectral Line Imaging Juergen Ott (ATNF) Juergen.Ott@csiro.au Topics Introduction to Spectral Lines Velocity Reference Frames Bandpass Calibration Continuum Subtraction Gibbs
More informationCoupled Sectorial Loop Antenna (CSLA) for Ultra Wideband Applications
Coupled Sectorial Loop Antenna (CSLA) for Ultra Wideband Applications N. Behdad and K. Sarabandi Presented by Nader Behdad at Antenna Application Symposium, Monticello, IL, Sep 2004 Email: behdad@ieee.org
More informationNuclear Magnetic Resonance (NMR)
California Institute of Technology Physics 77 Nuclear Magnetic Resonance (NMR) Eric D. Black September 27, 2005 1 Theory Read Section 14.4 of Shankar, Spin Dynamics, including the optional digression on
More informationElectromagnetic Spectrum
Electromagnetic Spectrum The electromagnetic radiation covers a vast spectrum of frequencies and wavelengths. This includes the very energetic gamma-rays radiation with a wavelength range from 0.005 1.4
More informationLecture notes on Waves/Spectra Noise, Correlations and.
Lecture notes on Waves/Spectra Noise, Correlations and. W. Gekelman Lecture 4, February 28, 2004 Our digital data is a function of time x(t) and can be represented as: () = a + ( a n t+ b n t) x t cos
More informationRF Systems I. Erk Jensen, CERN BE-RF
RF Systems I Erk Jensen, CERN BE-RF Introduction to Accelerator Physics, Prague, Czech Republic, 31 Aug 12 Sept 2014 Definitions & basic concepts db t-domain vs. ω-domain phasors 8th Sept, 2014 CAS Prague
More information1 ONE- and TWO-DIMENSIONAL HARMONIC OSCIL- LATIONS
SIMG-232 LABORATORY #1 Writeup Due 3/23/2004 (T) 1 ONE- and TWO-DIMENSIONAL HARMONIC OSCIL- LATIONS 1.1 Rationale: This laboratory (really a virtual lab based on computer software) introduces the concepts
More informationDFT: Discrete Fourier Transform & Linear Signal Processing
DFT: Discrete Fourier Transform & Linear Signal Processing 2 nd Year Electronics Lab IMPERIAL COLLEGE LONDON Table of Contents Equipment... 2 Aims... 2 Objectives... 2 Recommended Textbooks... 3 Recommended
More informationIn a typical biological sample the concentration of the solute is 1 mm or less. In many situations,
Water suppression n a typical biological sample the concentration of the solute is 1 mm or less. n many situations, the signals of interest are those of amide protons that exchange with the solvent water.
More informationPhasor. Phasor Diagram of a Sinusoidal Waveform
Phasor A phasor is a vector that has an arrow head at one end which signifies partly the maximum value of the vector quantity ( V or I ) and partly the end of the vector that rotates. Generally, vectors
More informationSystem analysis and signal processing
System analysis and signal processing with emphasis on the use of MATLAB PHILIP DENBIGH University of Sussex ADDISON-WESLEY Harlow, England Reading, Massachusetts Menlow Park, California New York Don Mills,
More informationUTA EE5380 PhD Diagnosis Exam (Fall 2011) Principles of Photonics and Optical Engineering
EE 5380 Fall 2011 PhD Diagnosis Exam ID: UTA EE5380 PhD Diagnosis Exam (Fall 2011) Principles of Photonics and Optical Engineering Instructions: Verify that your exam contains 7 pages (including the cover
More informationIntroduction to signals and systems
CHAPTER Introduction to signals and systems Welcome to Introduction to Signals and Systems. This text will focus on the properties of signals and systems, and the relationship between the inputs and outputs
More informationHideo Okawara s Mixed Signal Lecture Series. DSP-Based Testing Fundamentals 14 FIR Filter
Hideo Okawara s Mixed Signal Lecture Series DSP-Based Testing Fundamentals 14 FIR Filter Verigy Japan June 2009 Preface to the Series ADC and DAC are the most typical mixed signal devices. In mixed signal
More informationPhysics 319 Laboratory: Optics
1 Physics 319 Laboratory: Optics Birefringence II Objective: Previously, we have been concerned with the effect of linear polarizers on unpolarized and linearly polarized light. In this lab, we will explore
More information8.5 Modulation of Signals
8.5 Modulation of Signals basic idea and goals measuring atomic absorption without modulation measuring atomic absorption with modulation the tuned amplifier, diode rectifier and low pass the lock-in amplifier
More information9. Microwaves. 9.1 Introduction. Safety consideration
MW 9. Microwaves 9.1 Introduction Electromagnetic waves with wavelengths of the order of 1 mm to 1 m, or equivalently, with frequencies from 0.3 GHz to 0.3 THz, are commonly known as microwaves, sometimes
More informationLecture 7: Basics of magnetic resonance imaging (MRI): one dimensional Fourier imaging
Lecture 7: Basics of magnetic resonance imaging (MRI): one dimensional Fourier imaging Lecture aims to explain: 1. Basic aims of magnetic resonance imaging 2. Signal demodulation in magnetic resonance
More informationWhat are we looking at?
What are we looking at? What are our Goals: Accurate information to provide: Machinery Condition Monitoring Machinery Diagnostics Machinery Reliability Improvements Etc. Probe Coil Types 3000 and 7000
More informationDefinitions. Spectrum Analyzer
SIGNAL ANALYZERS Spectrum Analyzer Definitions A spectrum analyzer measures the magnitude of an input signal versus frequency within the full frequency range of the instrument. The primary use is to measure
More informationLong-distance propagation of short-wavelength spin waves. Liu et al.
Long-distance propagation of short-wavelength spin waves Liu et al. Supplementary Note 1. Characterization of the YIG thin film Supplementary fig. 1 shows the characterization of the 20-nm-thick YIG film
More informationFigure1. To construct a light pulse, the electric component of the plane wave should be multiplied with a bell shaped function.
Introduction The Electric field of a monochromatic plane wave is given by is the angular frequency of the plane wave. The plot of this function is given by a cosine function as shown in the following graph.
More informationLab 3.0. Pulse Shaping and Rayleigh Channel. Faculty of Information Engineering & Technology. The Communications Department
Faculty of Information Engineering & Technology The Communications Department Course: Advanced Communication Lab [COMM 1005] Lab 3.0 Pulse Shaping and Rayleigh Channel 1 TABLE OF CONTENTS 2 Summary...
More informationJoint Time/Frequency Analysis, Q Quality factor and Dispersion computation using Gabor-Morlet wavelets or Gabor-Morlet transform
Joint Time/Frequency, Computation of Q, Dr. M. Turhan (Tury Taner, Rock Solid Images Page: 1 Joint Time/Frequency Analysis, Q Quality factor and Dispersion computation using Gabor-Morlet wavelets or Gabor-Morlet
More informationPhysics 132 Quiz # 23
Name (please (please print) print) Physics 132 Quiz # 23 I. I. The The current in in an an ac ac circuit is is represented by by a phasor.the value of of the the current at at some time time t t is is
More informationHMBC 17. Goto. Introduction AVANCE User s Guide Bruker 185
Chapter HMBC 17 Introduction 17.1 Goto Heteronuclear Multiple Bond Correlation spectroscopy is a modified version of HMQC suitable for determining long-range 1 H- 13 C connectivity. This is useful in determining
More informationI am very pleased to teach this class again, after last year s course on electronics over the Summer Term. Based on the SOLE survey result, it is clear that the format, style and method I used worked with
More informationEE42: Running Checklist of Electronics Terms Dick White
EE42: Running Checklist of Electronics Terms 14.02.05 Dick White Terms are listed roughly in order of their introduction. Most definitions can be found in your text. Terms2 TERM Charge, current, voltage,
More informationR. J. Jones College of Optical Sciences OPTI 511L Fall 2017
R. J. Jones College of Optical Sciences OPTI 511L Fall 2017 Active Modelocking of a Helium-Neon Laser The generation of short optical pulses is important for a wide variety of applications, from time-resolved
More informationAntenna Engineering Lecture 3: Basic Antenna Parameters
Antenna Engineering Lecture 3: Basic Antenna Parameters ELC 405a Fall 2011 Department of Electronics and Communications Engineering Faculty of Engineering Cairo University 2 Outline 1 Radiation Pattern
More informationSignals and Systems Using MATLAB
Signals and Systems Using MATLAB Second Edition Luis F. Chaparro Department of Electrical and Computer Engineering University of Pittsburgh Pittsburgh, PA, USA AMSTERDAM BOSTON HEIDELBERG LONDON NEW YORK
More informationA Conceptual Tour of Pulsed NMR*
A Conceptual Tour of Pulsed NMR* Many nuclei, but not all, possess both a magnetic moment, µ, and an angular momentum, L. Such particles are said to have spin. When the angular momentum and magnetic moment
More informationSpectrum Analysis: The FFT Display
Spectrum Analysis: The FFT Display Equipment: Capstone, voltage sensor 1 Introduction It is often useful to represent a function by a series expansion, such as a Taylor series. There are other series representations
More informationEddy Current Testing (ET) Technique
Research Group Eddy Current Testing (ET) Technique Professor Pedro Vilaça * * Contacts: Address: Puumiehenkuja 3 (room 202), 02150 Espoo, Finland pedro.vilaca@aalto.fi October 2017 Contents Historical
More information8.2 Common Forms of Noise
8.2 Common Forms of Noise Johnson or thermal noise shot or Poisson noise 1/f noise or drift interference noise impulse noise real noise 8.2 : 1/19 Johnson Noise Johnson noise characteristics produced by
More informationLinear Time-Invariant Systems
Linear Time-Invariant Systems Modules: Wideband True RMS Meter, Audio Oscillator, Utilities, Digital Utilities, Twin Pulse Generator, Tuneable LPF, 100-kHz Channel Filters, Phase Shifter, Quadrature Phase
More informationEE 215 Semester Project SPECTRAL ANALYSIS USING FOURIER TRANSFORM
EE 215 Semester Project SPECTRAL ANALYSIS USING FOURIER TRANSFORM Department of Electrical and Computer Engineering Missouri University of Science and Technology Page 1 Table of Contents Introduction...Page
More informationS PG Course in Radio Communications. Orthogonal Frequency Division Multiplexing Yu, Chia-Hao. Yu, Chia-Hao 7.2.
S-72.4210 PG Course in Radio Communications Orthogonal Frequency Division Multiplexing Yu, Chia-Hao chyu@cc.hut.fi 7.2.2006 Outline OFDM History OFDM Applications OFDM Principles Spectral shaping Synchronization
More informationPHYS 352. FFT Convolution. More Advanced Digital Signal Processing Techniques
PHYS 352 More Advanced Digital Signal Processing Techniques FFT Convolution take a chunk of your signal (say N=128 samples) apply FFT to it multiply the frequency domain signal by your desired transfer
More informationDEPARTMENT OF CSE QUESTION BANK
DEPARTMENT OF CSE QUESTION BANK SUBJECT CODE: CS6304 SUBJECT NAME: ANALOG AND DIGITAL COMMUNICATION Part-A UNIT-I ANALOG COMMUNICATION 1.Define modulation? Modulation is a process by which some characteristics
More information2.1 BASIC CONCEPTS Basic Operations on Signals Time Shifting. Figure 2.2 Time shifting of a signal. Time Reversal.
1 2.1 BASIC CONCEPTS 2.1.1 Basic Operations on Signals Time Shifting. Figure 2.2 Time shifting of a signal. Time Reversal. 2 Time Scaling. Figure 2.4 Time scaling of a signal. 2.1.2 Classification of Signals
More informationAn EPR Primer 2. Basic EPR Theory 2.1. Introduction to Spectroscopy 2.1.1
An EPR Primer 2 This chapter is an introduction to the basic theory and practice of EPR spectroscopy. It gives you sufficient background to understand the following chapters. In addition, we strongly encourage
More informationSpatial coherency of earthquake-induced ground accelerations recorded by 100-Station of Istanbul Rapid Response Network
Spatial coherency of -induced ground accelerations recorded by 100-Station of Istanbul Rapid Response Network Ebru Harmandar, Eser Cakti, Mustafa Erdik Kandilli Observatory and Earthquake Research Institute,
More informationUNIT Explain the radiation from two-wire. Ans: Radiation from Two wire
UNIT 1 1. Explain the radiation from two-wire. Radiation from Two wire Figure1.1.1 shows a voltage source connected two-wire transmission line which is further connected to an antenna. An electric field
More informationInstruction manual for T3DS software. Tool for THz Time-Domain Spectroscopy. Release 4.0
Instruction manual for T3DS software Release 4.0 Table of contents 0. Setup... 3 1. Start-up... 5 2. Input parameters and delay line control... 6 3. Slow scan measurement... 8 4. Fast scan measurement...
More informationFourier and Wavelets
Fourier and Wavelets Why do we need a Transform? Fourier Transform and the short term Fourier (STFT) Heisenberg Uncertainty Principle The continues Wavelet Transform Discrete Wavelet Transform Wavelets
More informationFourier Theory & Practice, Part I: Theory (HP Product Note )
Fourier Theory & Practice, Part I: Theory (HP Product Note 54600-4) By: Robert Witte Hewlett-Packard Co. Introduction: This product note provides a brief review of Fourier theory, especially the unique
More information4 Waves Exam-style questions. AQA Physics. 1 a Define the amplitude of a wave. (1 mark) b i
1 a Define the amplitude of a wave. b i Other than electromagnetic radiation, give one example of a wave that is transverse. ii State one difference between a transverse wave and a longitudinal wave. c
More informationLecture 5: Polarisation of light 2
Lecture 5: Polarisation of light 2 Lecture aims to explain: 1. Circularly and elliptically polarised light 2. Optical retarders - Birefringence - Quarter-wave plate, half-wave plate Circularly and elliptically
More informationTheory of Telecommunications Networks
Theory of Telecommunications Networks Anton Čižmár Ján Papaj Department of electronics and multimedia telecommunications CONTENTS Preface... 5 1 Introduction... 6 1.1 Mathematical models for communication
More informationYour first NMR measurement
Your first NMR measurement Introduction Select 10mM water in D2O as NMR sample. The NMR spectrum of such sample consists of only two signals: the water signal and the peak of the reference (TSP). Follow
More informationSpectrum Analyzer TEN MINUTE TUTORIAL
Spectrum Analyzer TEN MINUTE TUTORIAL November 4, 2011 Summary The Spectrum Analyzer option allows users who are familiar with RF spectrum analyzers to start using the FFT with little or no concern about
More informationOverview ta3520 Introduction to seismics
Overview ta3520 Introduction to seismics Fourier Analysis Basic principles of the Seismic Method Interpretation of Raw Seismic Records Seismic Instrumentation Processing of Seismic Reflection Data Vertical
More informationELECTROMYOGRAPHY UNIT-4
ELECTROMYOGRAPHY UNIT-4 INTRODUCTION EMG is the study of muscle electrical signals. EMG is sometimes referred to as myoelectric activity. Muscle tissue conducts electrical potentials similar to the way
More informationLecture: Complex Exponentials
Lecture: Complex Exponentials 2009-2019, B.-P. Paris ECE 201: Intro to Signal Analysis 37 Introduction I The complex exponential signal is defined as x(t) =A exp(j(2pft + f)). I As with sinusoids, A, f,
More informationS1. Current-induced switching in the magnetic tunnel junction.
S1. Current-induced switching in the magnetic tunnel junction. Current-induced switching was observed at room temperature at various external fields. The sample is prepared on the same chip as that used
More informationDISCRETE FOURIER TRANSFORM AND FILTER DESIGN
DISCRETE FOURIER TRANSFORM AND FILTER DESIGN N. C. State University CSC557 Multimedia Computing and Networking Fall 2001 Lecture # 03 Spectrum of a Square Wave 2 Results of Some Filters 3 Notation 4 x[n]
More informationFIR/Convolution. Visulalizing the convolution sum. Convolution
FIR/Convolution CMPT 368: Lecture Delay Effects Tamara Smyth, tamaras@cs.sfu.ca School of Computing Science, Simon Fraser University April 2, 27 Since the feedforward coefficient s of the FIR filter are
More informationFunction Guide for the Fourier Transformation Package SPIRE-UOL-REP
Function Guide for the Fourier Transformation Package Prepared by: Peter Davis (University of Lethbridge) peter.davis@uleth.ca Andres Rebolledo (University of Lethbridge) andres.rebolledo@uleth.ca Trevor
More informationOptical Isolator Tutorial (Page 1 of 2) νlh, where ν, L, and H are as defined below. ν: the Verdet Constant, a property of the
Aspheric Optical Isolator Tutorial (Page 1 of 2) Function An optical isolator is a passive magneto-optic device that only allows light to travel in one direction. Isolators are used to protect a source
More informationPulses in Fibers. Advanced Lab Course. University of Bern Institute of Applied Physics Biomedical Photonics
Pulses in Fibers Advanced Lab Course University of Bern Institute of Applied Physics Biomedical Photonics September 2014 Contents 1 Theory 3 1.1 Electricity................................... 3 1.2 Optics.....................................
More informationIon Heating Arising from the Damping of Short Wavelength Fluctuations at the Edge of a Helicon Plasma Source
Ion Heating Arising from the Damping of Short Wavelength Fluctuations at the Edge of a Helicon Plasma Source Division of Plasma Physics American Physical Society October 2012 Providence, RI Earl Scime,
More informationSpectral Line II: Calibration and Analysis. Spectral Bandpass: Bandpass Calibration (cont d) Bandpass Calibration. Bandpass Calibration
Spectral Line II: Calibration and Analysis Bandpass Calibration Flagging Continuum Subtraction Imaging Visualization Analysis Spectral Bandpass: Spectral frequency response of antenna to a spectrally flat
More informationOptical Signal Processing
Optical Signal Processing ANTHONY VANDERLUGT North Carolina State University Raleigh, North Carolina A Wiley-Interscience Publication John Wiley & Sons, Inc. New York / Chichester / Brisbane / Toronto
More informationTHE SINUSOIDAL WAVEFORM
Chapter 11 THE SINUSOIDAL WAVEFORM The sinusoidal waveform or sine wave is the fundamental type of alternating current (ac) and alternating voltage. It is also referred to as a sinusoidal wave or, simply,
More informationGradients. Effects of B0 gradients on transverse magnetisation Similar to figure 10 of Sattler review Progr. NMR 34 (1999), 93
Gradients 1. What are gradients? Modern high-resolution NMR probes contain -besides the RF coils - additional coils that can be fed a DC current. The coils are built so that a pulse (~1 ms long) of DC
More informationElectron Spin Resonance v2.0
Electron Spin Resonance v2.0 Background. This experiment measures the dimensionless g-factor (g s ) of an unpaired electron using the technique of Electron Spin Resonance, also known as Electron Paramagnetic
More informationPhase-Sensitive Detection
Concepts in Magnetic Resonance, 1990, 2, 181-195 Part 11: Quadrature Phase Detection Daniel D. Traficante ¶nems of Chemisby and Medicinal Chemicey and NMR Concepts univenily of Rhode s m Kingstom,
More informationCircuit Analysis-II. Circuit Analysis-II Lecture # 2 Wednesday 28 th Mar, 18
Circuit Analysis-II Angular Measurement Angular Measurement of a Sine Wave ü As we already know that a sinusoidal voltage can be produced by an ac generator. ü As the windings on the rotor of the ac generator
More informationINTERNATIONAL JOURNAL OF PURE AND APPLIED RESEARCH IN ENGINEERING AND TECHNOLOGY
INTERNATIONAL JOURNAL OF PURE AND APPLIED RESEARCH IN ENGINEERING AND TECHNOLOGY A PATH FOR HORIZING YOUR INNOVATIVE WORK STUDY OF THE BASICS OF SPECTRUM ANALYZER AND PERSPECTIVES MONALI CHAUDHARI 1, VAISHALI
More informationAgilent Time Domain Analysis Using a Network Analyzer
Agilent Time Domain Analysis Using a Network Analyzer Application Note 1287-12 0.0 0.045 0.6 0.035 Cable S(1,1) 0.4 0.2 Cable S(1,1) 0.025 0.015 0.005 0.0 1.0 1.5 2.0 2.5 3.0 3.5 4.0 Frequency (GHz) 0.005
More informationIMAC 27 - Orlando, FL Shaker Excitation
IMAC 27 - Orlando, FL - 2009 Peter Avitabile UMASS Lowell Marco Peres The Modal Shop 1 Dr. Peter Avitabile Objectives of this lecture: Overview some shaker excitation techniques commonly employed in modal
More informationOutline. Motivation Experimental Set-Up Theory behind the set-up Results Acknowledgements
Outline Motivation Experimental Set-Up Theory behind the set-up Results Acknowledgements Motivation Attosecond pulses could be used to study time-dependence of atomic dynamics. Greater control of pulse
More informationIMAGE PROCESSING (RRY025) THE CONTINUOUS 2D FOURIER TRANSFORM
IMAGE PROCESSING (RRY5) THE CONTINUOUS D FOURIER TRANSFORM INTRODUCTION A vital tool in image processing. Also a prototype of other image transforms, cosine, Wavelet etc. Applications Image Filtering -
More information(N)MR Imaging. Lab Course Script. FMP PhD Autumn School. Location: C81, MRI Lab B0.03 (basement) Instructor: Leif Schröder. Date: November 3rd, 2010
(N)MR Imaging Lab Course Script FMP PhD Autumn School Location: C81, MRI Lab B0.03 (basement) Instructor: Leif Schröder Date: November 3rd, 2010 1 Purpose: Understanding the basic principles of MR imaging
More informationProblems from the 3 rd edition
(2.1-1) Find the energies of the signals: a) sin t, 0 t π b) sin t, 0 t π c) 2 sin t, 0 t π d) sin (t-2π), 2π t 4π Problems from the 3 rd edition Comment on the effect on energy of sign change, time shifting
More informationExtending Vector Signal Analysis to 26.5 GHz with 20 MHz Information Bandwidth Product Note
H Extending Vector Signal Analysis to 26.5 GHz with 20 MHz Information Bandwidth Product Note 89400-13 The HP 89400 series vector signal analyzers provide unmatched signal analysis capabilities from traditional
More information