Chapter Three Theoretical Description Of Stochastic Resonance 24
|
|
- Sheena Powell
- 6 years ago
- Views:
Transcription
1 Table of Contents List of Abbreviations and Symbols 5 Chapter One Introduction The Phenomenon of the Stochastic Resonance The Purpose of the Study 10 Chapter Two The Experimental Set-up The Electric Circuit Experimental Realisation Methods of Signal Characterisation Stochastic Resonance Measures Spectral Amplification Signal-to-Noise Ratio Experimental Set-up 19 Chapter Three Theoretical Description Of Stochastic Resonance Effect Basics System with Double-well Potential System Response Stochastic Resonance Characteristics Spectral Amplification Signal-to-Noise Ratio Stochastic Resonance in Continuous Bistable System Fokker-Planck Description Floquet Approach Expressions for Stochastic Resonance Characteristics Expression for Spectral Amplification 37
2 Expression for Signal-to-Noise Ratio Results of Simulations Intrawell Motion Contribution Linear Response Approximation Concluding Remarks Ferroelectric TGS Crystal as a System Displaying Stochastic Resonance Frequency Scaling 47 Chapter Four Experimental Results Signatures of Stochastic Resonance Synchronisation and Signal Enhancement Behaviour of Spectral Amplification Behaviour of Signal-to-Noise Ratio Discussion Characterisation of Stochastic Resonance Frequency Dependences Discussion Amplitude Dependences Discussion Temperature Dependence of Stochastic Resonance Behaviour Behaviour of Stochastic Resonance Measures at Different Temperatures of Ferroelectric TGS Frequency Scaling Discussion 77 Chapter Five Conclusions and Outlook Outlook 81 References 83
3 5 List of Abbreviations and Symbols: A surface area A 0 amplitude of periodic modulation A A ~ 0 0 = ax m scaled amplitude a,b parameters of double-well potential AS C 0 C F c k d D D m asymptotic linear capacitance ferroelectric capacitance Fourier coefficient sample thickness noise intensity noise intensity that maximises system response D D ~ = scaled noise intensity 2 ax m E electric field strength eq. equation f frequency f ( x ) = V ( x ) / m scaled first derivative of the potential V(x) g n H(t) i expansion coefficient Heaviside step function imaginary unit k, m, n indexes 0 K xx ( t) correlation function
4 6 L 0 (t) unperturbed Fokker-Planck operator L ext (t) Fokker-Planck operator of periodic perturbation L * (t) adjoint Fokker-Planck operator m mass M n p {p µ } Floquet modes complex valued amplitudes of the system response probability density P Ρ(X,t Y, s) P P 1 P A P n Q polarisation transition probability density power integrated power of the delta-like peak at the frequency f=ω total power of the modulation signal in the absence of noise integrated power of δ-peaks of the n-th frequency component electric charge Q F r K R S(ω) S N (ω) SNR t, s, τ time t 0 electric charge of nonlinear capacitance C F Kramer s rate ohmic resistance output spectral density spectral density of noise signal-to-noise ratio initial time ~ at t = scaled time γ T T K T Ω TGS period period of Kramer s hopping period of periodic modulation triglycine sulfate C 0 voltage drop over C 0 C F voltage drop over C F G R driving voltage (periodic modulation) voltage drop over R
5 7 v V(x) V(x) x(t) x 0 =x(t 0 ) x m velocity double-well potential height of the potential barrier one-dimensional time-dependent coordinate initial condition coordinate of the potential minima x (D) periodic component of the system response x x~ = scaled variable x δx(t) X(ω) x m X(t), Y(s) Z χ(t) χ(ω) δ φ γ η ϕ λ n system response within linear response approximation Fourier transform of x(t) state vectors impedance response function Fourier transform of χ(t) delta-function phase shift viscous friction spectral amplification phase eigenvalue of Fokker-Planck operator µ Floquet eigenvalue Θ Θ τ smpl ω 0 ω k, ω n Ω temperature accuracy of temperature measurement sample rate angular frequency discrete angular frequency angular frequency of external periodic modulation ~ Ω Ω = γ scaled angular frequency a ξ(t) Gaussian white noise
Stochastic Resonance in Ferroelectric TGS Crystals
Stochastic Resonance in Ferroelectric TGS Crystals Dissertation zur Erlangung des akademischen Grades doctor rerum naturalium (Dr. rer. nat.) vorgelegt der Mathematisch-Naturwissenschaftlich-Technischen
More informationStochastic resonance Evgeny Bogomolny ID
Non-linear dynamics project Guided by prof. Y.Zarmi Stochastic resonance Evgeny Bogomolny ID 306654559 Preface Stochastic resonance (SR) provides a intriguing example of a noise-induced transition in a
More informationAnalysis of Stochastic Resonance Phenomenon in Wind Induced Vibration of a Girder POSPÍŠIL Stanislav 1,a and NÁPRSTEK Jiří 1,b
Applied Mechanics and Materials Online: 2014-08-18 ISSN: 1662-7482, Vol. 617, pp 285-290 doi:10.4028/www.scientific.net/amm.617.285 2014 Trans Tech Publications, Switzerland Analysis of Stochastic Resonance
More information5 Applying the Fokker-Planck equation
5 Applying the Fokker-Planck equation We begin with one-dimensional examples, keeping g = constant. Recall: the FPE for the Langevin equation with η(t 1 )η(t ) = κδ(t 1 t ) is = f(x) + g(x)η(t) t = x [f(x)p
More informationAC Circuits Homework Set
Problem 1. In an oscillating LC circuit in which C=4.0 μf, the maximum potential difference across the capacitor during the oscillations is 1.50 V and the maximum current through the inductor is 50.0 ma.
More informationarxiv: v1 [nlin.cd] 22 Aug 2016
The Two Dynamical States of a Driven Underdamped Classical Pendulum: An Analog Simulation Experiment Ivan Skhem Sawkmie and Mangal C. Mahato Department of Physics, North-Eastern Hill University, Shillong-793022,
More informationHandbook of Stochastic Methods
C. W. Gardiner Handbook of Stochastic Methods for Physics, Chemistry and the Natural Sciences Third Edition With 30 Figures Springer Contents 1. A Historical Introduction 1 1.1 Motivation I 1.2 Some Historical
More informationThe correlation between stochastic resonance and the average phase-synchronization time of a bistable system driven by colour-correlated noises
Chin. Phys. B Vol. 19, No. 1 (010) 01050 The correlation between stochastic resonance and the average phase-synchronization time of a bistable system driven by colour-correlated noises Dong Xiao-Juan(
More informationEQUATION LANGEVIN. Physics, Chemistry and Electrical Engineering. World Scientific. With Applications to Stochastic Problems in. William T.
SHANGHAI HONG WorlrfScientific Series krtonttimfjorary Chemical Physics-Vol. 27 THE LANGEVIN EQUATION With Applications to Stochastic Problems in Physics, Chemistry and Electrical Engineering Third Edition
More informationUniversity of Jordan Faculty of Engineering & Technology Electric Power Engineering Department
University of Jordan Faculty of Engineering & Technology Electric Power Engineering Department EE471: Electrical Machines-II Tutorial # 2: 3-ph Induction Motor/Generator Question #1 A 100 hp, 60-Hz, three-phase
More informationElectromagnetic Oscillations and Alternating Current. 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3.
Electromagnetic Oscillations and Alternating Current 1. Electromagnetic oscillations and LC circuit 2. Alternating Current 3. RLC circuit in AC 1 RL and RC circuits RL RC Charging Discharging I = emf R
More information0-2 Operations with Complex Numbers
Simplify. 1. i 10 2. i 2 + i 8 3. i 3 + i 20 4. i 100 5. i 77 esolutions Manual - Powered by Cognero Page 1 6. i 4 + i 12 7. i 5 + i 9 8. i 18 Simplify. 9. (3 + 2i) + ( 4 + 6i) 10. (7 4i) + (2 3i) 11.
More informationRLC Series Circuit. We can define effective resistances for capacitors and inductors: 1 = Capacitive reactance:
RLC Series Circuit In this exercise you will investigate the effects of changing inductance, capacitance, resistance, and frequency on an RLC series AC circuit. We can define effective resistances for
More information1 Phasors and Alternating Currents
Physics 4 Chapter : Alternating Current 0/5 Phasors and Alternating Currents alternating current: current that varies sinusoidally with time ac source: any device that supplies a sinusoidally varying potential
More information0-2 Operations with Complex Numbers
Simplify. 1. i 10 1 2. i 2 + i 8 0 3. i 3 + i 20 1 i esolutions Manual - Powered by Cognero Page 1 4. i 100 1 5. i 77 i 6. i 4 + i 12 2 7. i 5 + i 9 2i esolutions Manual - Powered by Cognero Page 2 8.
More informationStochastic resonance in a monostable system driven by square-wave signal and dichotomous noise
Stochastic resonance in a monostable system driven by square-wave signal and dichotomous noise Guo Feng( 郭锋 ) a), Luo Xiang-Dong( 罗向东 ) a), Li Shao-Fu( 李少甫 ) a), and Zhou Yu-Rong( 周玉荣 ) b) a) School of
More informationLINEAR RESPONSE THEORY
MIT Department of Chemistry 5.74, Spring 5: Introductory Quantum Mechanics II Instructor: Professor Andrei Tokmakoff p. 8 LINEAR RESPONSE THEORY We have statistically described the time-dependent behavior
More informationThe Kramers problem and first passage times.
Chapter 8 The Kramers problem and first passage times. The Kramers problem is to find the rate at which a Brownian particle escapes from a potential well over a potential barrier. One method of attack
More informationFile name: Supplementary Information Description: Supplementary Figures, Supplementary Notes and Supplementary References
File name: Supplementary Information Description: Supplementary Figures, Supplementary Notes and Supplementary References File name: Peer Review File Description: Optical frequency (THz) 05. 0 05. 5 05.7
More informationLinear and nonlinear approximations for periodically driven bistable systems
Invited Paper Linear and nonlinear approximations for periodically driven bistable systems Alexander A. Dubkov a, Bernardo Spagnolo b, and Davide Valenti b a Radiophysics Department, Nizhni Novgorod State
More informationNonlinear Stochastic Resonance with subthreshold rectangular pulses arxiv:cond-mat/ v1 [cond-mat.stat-mech] 15 Jan 2004.
Nonlinear Stochastic Resonance with subthreshold rectangular pulses arxiv:cond-mat/4163v1 [cond-mat.stat-mech] 15 Jan 4 Jesús Casado-Pascual, José Gómez-Ordóñez, and Manuel Morillo Física Teórica, Universidad
More informationSome of the different forms of a signal, obtained by transformations, are shown in the figure. jwt e z. jwt z e
Transform methods Some of the different forms of a signal, obtained by transformations, are shown in the figure. X(s) X(t) L - L F - F jw s s jw X(jw) X*(t) F - F X*(jw) jwt e z jwt z e X(nT) Z - Z X(z)
More informationEscape Problems & Stochastic Resonance
Escape Problems & Stochastic Resonance 18.S995 - L08 & 09 dunkel@mit.edu Examples Illustration by J.P. Cartailler. Copyright 2007, Symmation LLC. transport & evolution: stochastic escape problems http://evolutionarysystemsbiology.org/intro/
More informationExercise sheet 3: Random walk and diffusion equation, the Wiener-Khinchin theorem, correlation function and power spectral density
AMSI (217) Stochastic Equations and Processes in Physics and Biology Exercise sheet 3: Random walk and diffusion equation, the Wiener-Khinchin theorem, correlation function and power spectral density 1.
More informationDetection and Parameter Estimation of LFM Signal Based on Stochastic Resonance
nd International Conference on Networking and Information Technology IPCSIT vol.7 () () IACSIT Press, Singapore Detection and Parameter Estimation of LFM Signal Based on Stochastic Resonance Xiaomin Wang
More informationLecture 1: Pragmatic Introduction to Stochastic Differential Equations
Lecture 1: Pragmatic Introduction to Stochastic Differential Equations Simo Särkkä Aalto University, Finland (visiting at Oxford University, UK) November 13, 2013 Simo Särkkä (Aalto) Lecture 1: Pragmatic
More informationSTOCHASTIC PROCESSES IN PHYSICS AND CHEMISTRY
STOCHASTIC PROCESSES IN PHYSICS AND CHEMISTRY Third edition N.G. VAN KAMPEN Institute for Theoretical Physics of the University at Utrecht ELSEVIER Amsterdam Boston Heidelberg London New York Oxford Paris
More information2 Lyapunov Stability. x(0) x 0 < δ x(t) x 0 < ɛ
1 2 Lyapunov Stability Whereas I/O stability is concerned with the effect of inputs on outputs, Lyapunov stability deals with unforced systems: ẋ = f(x, t) (1) where x R n, t R +, and f : R n R + R n.
More information3. ESTIMATION OF SIGNALS USING A LEAST SQUARES TECHNIQUE
3. ESTIMATION OF SIGNALS USING A LEAST SQUARES TECHNIQUE 3.0 INTRODUCTION The purpose of this chapter is to introduce estimators shortly. More elaborated courses on System Identification, which are given
More informationHandout 11: AC circuit. AC generator
Handout : AC circuit AC generator Figure compares the voltage across the directcurrent (DC) generator and that across the alternatingcurrent (AC) generator For DC generator, the voltage is constant For
More informationLINEAR SYSTEMS. J. Elder PSYC 6256 Principles of Neural Coding
LINEAR SYSTEMS Linear Systems 2 Neural coding and cognitive neuroscience in general concerns input-output relationships. Inputs Light intensity Pre-synaptic action potentials Number of items in display
More informationLinear Systems Theory
ME 3253 Linear Systems Theory Review Class Overview and Introduction 1. How to build dynamic system model for physical system? 2. How to analyze the dynamic system? -- Time domain -- Frequency domain (Laplace
More informationQuantifying stochastic resonance: theory versus experiment
Erschienen in: Journal of Physics : Condensed Matter ; 17 (2005), 47. - S. S3795-S3809 https://dx.doi.org/10.1088/0953-8984/17/47/011 Quantifying stochastic resonance: theory versus experiment Mykhaylo
More informationFundamentals of Noise
Fundamentals of Noise V.Vasudevan, Department of Electrical Engineering, Indian Institute of Technology Madras Noise in resistors Random voltage fluctuations across a resistor Mean square value in a frequency
More information2A1H Time-Frequency Analysis II
2AH Time-Frequency Analysis II Bugs/queries to david.murray@eng.ox.ac.uk HT 209 For any corrections see the course page DW Murray at www.robots.ox.ac.uk/ dwm/courses/2tf. (a) A signal g(t) with period
More informationElectrical Circuits Lab Series RC Circuit Phasor Diagram
Electrical Circuits Lab. 0903219 Series RC Circuit Phasor Diagram - Simple steps to draw phasor diagram of a series RC circuit without memorizing: * Start with the quantity (voltage or current) that is
More informationNANOSCALE SCIENCE & TECHNOLOGY
. NANOSCALE SCIENCE & TECHNOLOGY V Two-Level Quantum Systems (Qubits) Lecture notes 5 5. Qubit description Quantum bit (qubit) is an elementary unit of a quantum computer. Similar to classical computers,
More informationStochastic resonance: non-robust and robust tuning notions
Stochastic resonance: non-robust and robust tuning notions S. Herrmann 1 P. Imkeller I. Pavlyukevich 3 14th February 003 Abstract We consider a dynamical system describing the diffusive motion of a particle
More informationDynamic Modeling. For the mechanical translational system shown in Figure 1, determine a set of first order
QUESTION 1 For the mechanical translational system shown in, determine a set of first order differential equations describing the system dynamics. Identify the state variables and inputs. y(t) x(t) k m
More informationpickup from external sources unwanted feedback RF interference from system or elsewhere, power supply fluctuations ground currents
Noise What is NOISE? A definition: Any unwanted signal obscuring signal to be observed two main origins EXTRINSIC NOISE examples... pickup from external sources unwanted feedback RF interference from system
More informationFourier Analysis and Power Spectral Density
Chapter 4 Fourier Analysis and Power Spectral Density 4. Fourier Series and ransforms Recall Fourier series for periodic functions for x(t + ) = x(t), where x(t) = 2 a + a = 2 a n = 2 b n = 2 n= a n cos
More informationReview of Linear Time-Invariant Network Analysis
D1 APPENDIX D Review of Linear Time-Invariant Network Analysis Consider a network with input x(t) and output y(t) as shown in Figure D-1. If an input x 1 (t) produces an output y 1 (t), and an input x
More informationA path integral approach to the Langevin equation
A path integral approach to the Langevin equation - Ashok Das Reference: A path integral approach to the Langevin equation, A. Das, S. Panda and J. R. L. Santos, arxiv:1411.0256 (to be published in Int.
More informationApplied Probability and Stochastic Processes
Applied Probability and Stochastic Processes In Engineering and Physical Sciences MICHEL K. OCHI University of Florida A Wiley-Interscience Publication JOHN WILEY & SONS New York - Chichester Brisbane
More informationLearnabout Electronics - AC Theory
Learnabout Electronics - AC Theory Facts & Formulae for AC Theory www.learnabout-electronics.org Contents AC Wave Values... 2 Capacitance... 2 Charge on a Capacitor... 2 Total Capacitance... 2 Inductance...
More informationTHE problem of phase noise and its influence on oscillators
IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS II: EXPRESS BRIEFS, VOL. 54, NO. 5, MAY 2007 435 Phase Diffusion Coefficient for Oscillators Perturbed by Colored Noise Fergal O Doherty and James P. Gleeson Abstract
More informationElectrodynamics Qualifier Examination
Electrodynamics Qualifier Examination January 10, 2007 1. This problem deals with magnetostatics, described by a time-independent magnetic field, produced by a current density which is divergenceless,
More informationarxiv:q-bio/ v2 [q-bio.pe] 12 Mar 2004
DISCRETE AND CONTINUOUS Website: http://aimsciences.org DYNAMICAL SYSTEMS Volume, Number 0, pp. NOISE IN ECOSYSTEMS: A SHORT REVIEW arxiv:q-bio/0403004v2 [q-bio.pe] 12 Mar 2004 B. Spagnolo, D. Valenti,
More informationSynchronization of Limit Cycle Oscillators by Telegraph Noise. arxiv: v1 [cond-mat.stat-mech] 5 Aug 2014
Synchronization of Limit Cycle Oscillators by Telegraph Noise Denis S. Goldobin arxiv:148.135v1 [cond-mat.stat-mech] 5 Aug 214 Department of Physics, University of Potsdam, Postfach 61553, D-14415 Potsdam,
More informationPhysics 1214 Chapter 19: Current, Resistance, and Direct-Current Circuits
Physics 1214 Chapter 19: Current, Resistance, and Direct-Current Circuits 1 Current current: (also called electric current) is an motion of charge from one region of a conductor to another. Current When
More informationES 272 Assignment #2. in,3
ES 272 Assignment #2 Due: March 14th, 2014; 5pm sharp, in the dropbox outside MD 131 (Donhee Ham office) Instructor: Donhee Ham (copyright c 2014 by D. Ham) (Problem 1) The kt/c Noise (50pt) Imagine an
More informationChapter 10: Sinusoidal Steady-State Analysis
Chapter 10: Sinusoidal Steady-State Analysis 1 Objectives : sinusoidal functions Impedance use phasors to determine the forced response of a circuit subjected to sinusoidal excitation Apply techniques
More informationExam. Matrikelnummer: Points. Question Bonus. Total. Grade. Information Theory and Signal Reconstruction Summer term 2013
Exam Name: Matrikelnummer: Question 1 2 3 4 5 Bonus Points Total Grade 1/6 Question 1 You are traveling to the beautiful country of Markovia. Your travel guide tells you that the weather w i in Markovia
More informationSTABILITY ANALYSIS OF DYNAMIC SYSTEMS
C. Melchiorri (DEI) Automatic Control & System Theory 1 AUTOMATIC CONTROL AND SYSTEM THEORY STABILITY ANALYSIS OF DYNAMIC SYSTEMS Claudio Melchiorri Dipartimento di Ingegneria dell Energia Elettrica e
More informationMODULE-4 RESONANCE CIRCUITS
Introduction: MODULE-4 RESONANCE CIRCUITS Resonance is a condition in an RLC circuit in which the capacitive and inductive Reactance s are equal in magnitude, there by resulting in purely resistive impedance.
More informationIn-class exercises Day 1
Physics 4488/6562: Statistical Mechanics http://www.physics.cornell.edu/sethna/teaching/562/ Material for Week 11 Exercises due Mon Apr 16 Last correction at April 16, 2018, 11:19 am c 2018, James Sethna,
More informationUCSD ECE153 Handout #40 Prof. Young-Han Kim Thursday, May 29, Homework Set #8 Due: Thursday, June 5, 2011
UCSD ECE53 Handout #40 Prof. Young-Han Kim Thursday, May 9, 04 Homework Set #8 Due: Thursday, June 5, 0. Discrete-time Wiener process. Let Z n, n 0 be a discrete time white Gaussian noise (WGN) process,
More informationAdvanced Quantum Mechanics
Advanced Quantum Mechanics Rajdeep Sensarma sensarma@theory.tifr.res.in Quantum Dynamics Lecture #2 Recap of Last Class Schrodinger and Heisenberg Picture Time Evolution operator/ Propagator : Retarded
More informationTheory of bifurcation amplifiers utilizing the nonlinear dynamical response of an optically damped mechanical oscillator
Theory of bifurcation amplifiers utilizing the nonlinear dynamical response of an optically damped mechanical oscillator Research on optomechanical systems is of relevance to gravitational wave detection
More informationFeature extraction 1
Centre for Vision Speech & Signal Processing University of Surrey, Guildford GU2 7XH. Feature extraction 1 Dr Philip Jackson Cepstral analysis - Real & complex cepstra - Homomorphic decomposition Filter
More informationAmplitude and Phase A(0) 2. We start with the Fourier series representation of X(t) in real notation: n=1
VI. Power Spectra Amplitude and Phase We start with the Fourier series representation of X(t) in real notation: A() X(t) = + [ A(n) cos(nωt) + B(n) sin(nωt)] 2 n=1 he waveform of the observed segment exactly
More informationJinki Kim Department of Mechanical Engineering University of Michigan
Bistable and Adaptive Piezoelectric Circuitry for Impedance-Based Structural Health Monitoring Jinki Kim Department of Mechanical Engineering University of Michigan April 20 2017 Outline of the Presentation
More informationChapter 33. Alternating Current Circuits
Chapter 33 Alternating Current Circuits 1 Capacitor Resistor + Q = C V = I R R I + + Inductance d I Vab = L dt AC power source The AC power source provides an alternative voltage, Notation - Lower case
More informationmywbut.com Lesson 16 Solution of Current in AC Parallel and Seriesparallel
esson 6 Solution of urrent in Parallel and Seriesparallel ircuits n the last lesson, the following points were described:. How to compute the total impedance/admittance in series/parallel circuits?. How
More informationSingle-Time-Constant (STC) Circuits This lecture is given as a background that will be needed to determine the frequency response of the amplifiers.
Single-Time-Constant (STC) Circuits This lecture is given as a background that will be needed to determine the frequency response of the amplifiers. Objectives To analyze and understand STC circuits with
More informationEE221 Circuits II. Chapter 14 Frequency Response
EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active
More informationarxiv:nlin/ v1 [nlin.ps] 17 Jun 2005
Stochastic Resonance in Underdamped, Bistable Systems arxiv:nlin/0506039v1 [nlin.ps] 17 Jun 2005 Rajarshi Ray a,b and Supratim Sengupta c,d a Tata Institute of Fundamental Research, Homi Bhabha Road, Mumbai
More informationRLC Circuits. 1 Introduction. 1.1 Undriven Systems. 1.2 Driven Systems
RLC Circuits Equipment: Capstone, 850 interface, RLC circuit board, 4 leads (91 cm), 3 voltage sensors, Fluke mulitmeter, and BNC connector on one end and banana plugs on the other Reading: Review AC circuits
More informationHandbook of Stochastic Methods
Springer Series in Synergetics 13 Handbook of Stochastic Methods for Physics, Chemistry and the Natural Sciences von Crispin W Gardiner Neuausgabe Handbook of Stochastic Methods Gardiner schnell und portofrei
More informationEE221 Circuits II. Chapter 14 Frequency Response
EE22 Circuits II Chapter 4 Frequency Response Frequency Response Chapter 4 4. Introduction 4.2 Transfer Function 4.3 Bode Plots 4.4 Series Resonance 4.5 Parallel Resonance 4.6 Passive Filters 4.7 Active
More informationVibrational resonance
Published in J. Phys. A: Math. Gen. 33, L433 L438 (2000). LETTER TO THE EDITOR Vibrational resonance P S Landa andpvemcclintock Department of Physics, Lomonosov Moscow State University, 119899 Moscow,
More informationω 0 = 2π/T 0 is called the fundamental angular frequency and ω 2 = 2ω 0 is called the
he ime-frequency Concept []. Review of Fourier Series Consider the following set of time functions {3A sin t, A sin t}. We can represent these functions in different ways by plotting the amplitude versus
More informationΑ Dispersion Relation for Open Spiral Galaxies
J. Astrophys. Astr. (1980) 1, 79 95 Α Dispersion Relation for Open Spiral Galaxies G. Contopoulos Astronomy Department, University of Athens, Athens, Greece Received 1980 March 20; accepted 1980 April
More informationStochastic models in biology and their deterministic analogues
Stochastic models in biology and their deterministic analogues Alan McKane Theory Group, School of Physics and Astronomy, University of Manchester Newton Institute, May 2, 2006 Stochastic models in biology
More informationContents. I Background 1. Contents... Preface... Acknowledgments... The Blind Men and the Elephant... xxi. History of Impedance Spectroscopy...
Contents Contents...................................... Preface....................................... Acknowledgments................................. v xv xix The Blind Men and the Elephant.......................
More informationReview: control, feedback, etc. Today s topic: state-space models of systems; linearization
Plan of the Lecture Review: control, feedback, etc Today s topic: state-space models of systems; linearization Goal: a general framework that encompasses all examples of interest Once we have mastered
More informationOptimal driving waveform for the overdamped, rocking ratchets
Optimal driving waveform for the overdamped, rocking ratchets Maria Laura Olivera Instituto de Ciencias de la Universidad Nacional de General Sarmiento. Buenos Aires Argentina Directors: R. Álvarez-Nodarse
More informationCast of Characters. Some Symbols, Functions, and Variables Used in the Book
Page 1 of 6 Cast of Characters Some s, Functions, and Variables Used in the Book Digital Signal Processing and the Microcontroller by Dale Grover and John R. Deller ISBN 0-13-081348-6 Prentice Hall, 1998
More information2A1H Time-Frequency Analysis II Bugs/queries to HT 2011 For hints and answers visit dwm/courses/2tf
Time-Frequency Analysis II (HT 20) 2AH 2AH Time-Frequency Analysis II Bugs/queries to david.murray@eng.ox.ac.uk HT 20 For hints and answers visit www.robots.ox.ac.uk/ dwm/courses/2tf David Murray. A periodic
More informationStudy on Tire-attached Energy Harvester for Lowspeed Actual Vehicle Driving
Journal of Physics: Conference Series PAPER OPEN ACCESS Study on Tire-attached Energy Harvester for Lowspeed Actual Vehicle Driving To cite this article: Y Zhang et al 15 J. Phys.: Conf. Ser. 66 116 Recent
More informationMATHEMATICAL MODELING OF DYNAMIC SYSTEMS
MTHEMTIL MODELIN OF DYNMI SYSTEMS Mechanical Translational System 1. Spring x(t) k F S (t) k x(t) x i (t) k x o (t) 2. Damper x(t) x i (t) x o (t) c c 3. Mass x(t) F(t) m EXMPLE I Produce the block diagram
More informationModule 13: Network Analysis and Directional Couplers
Module 13: Network Analysis and Directional Couplers 13.2 Network theory two port networks, S-parameters, Z-parameters, Y-parameters The study of two port networks is important in the field of electrical
More informationTHREE-BODY INTERACTIONS DRIVE THE TRANSITION TO POLAR ORDER IN A SIMPLE FLOCKING MODEL
THREE-BODY INTERACTIONS DRIVE THE TRANSITION TO POLAR ORDER IN A SIMPLE FLOCKING MODEL Purba Chatterjee and Nigel Goldenfeld Department of Physics University of Illinois at Urbana-Champaign Flocking in
More informationENSC327 Communications Systems 2: Fourier Representations. School of Engineering Science Simon Fraser University
ENSC37 Communications Systems : Fourier Representations School o Engineering Science Simon Fraser University Outline Chap..5: Signal Classiications Fourier Transorm Dirac Delta Function Unit Impulse Fourier
More information7.7 The Schottky Formula for Shot Noise
110CHAPTER 7. THE WIENER-KHINCHIN THEOREM AND APPLICATIONS 7.7 The Schottky Formula for Shot Noise On p. 51, we found that if one averages τ seconds of steady electron flow of constant current then the
More informationThis is a Gaussian probability centered around m = 0 (the most probable and mean position is the origin) and the mean square displacement m 2 = n,or
Physics 7b: Statistical Mechanics Brownian Motion Brownian motion is the motion of a particle due to the buffeting by the molecules in a gas or liquid. The particle must be small enough that the effects
More informationSignals and Spectra (1A) Young Won Lim 11/26/12
Signals and Spectra (A) Copyright (c) 202 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version.2 or any later
More information16. Working with the Langevin and Fokker-Planck equations
16. Working with the Langevin and Fokker-Planck equations In the preceding Lecture, we have shown that given a Langevin equation (LE), it is possible to write down an equivalent Fokker-Planck equation
More informationI. Impedance of an R-L circuit.
I. Impedance of an R-L circuit. [For inductor in an AC Circuit, see Chapter 31, pg. 1024] Consider the R-L circuit shown in Figure: 1. A current i(t) = I cos(ωt) is driven across the circuit using an AC
More informationECE 6340 Fall Homework 2. Please do the following problems (you may do the others for practice if you wish): Probs. 1, 2, 3, 4, 5, 6, 7, 10, 12
ECE 634 Fall 16 Homework Please do the following problems (you may do the others for practice if you wish: Probs. 1,, 3, 4, 5, 6, 7, 1, 1 1 Consider two parallel infinite wires in free space each carrying
More informationLecture (5) Power Factor,threephase circuits, and Per Unit Calculations
Lecture (5) Power Factor,threephase circuits, and Per Unit Calculations 5-1 Repeating the Example on Power Factor Correction (Given last Class) P? Q? S? Light Motor From source 1000 volts @ 60 Htz 10kW
More informationarxiv: v1 [physics.flu-dyn] 4 Jul 2015
Comments on turbulence theory by Qian and by Edwards and McComb R. V. R. Pandya Department of Mechanical Engineering, arxiv:1507.0114v1 [physics.flu-dyn] 4 Jul 015 University of Puerto Rico at Mayaguez,
More informationPY3107 Experimental Physics II
PY3107 Experimental Physics II ock-in Amplifiers MP aughan and F Peters Related Experiments ock-in ab ignal processing and phase sensitive detection using a lock-in amplifier The problem The signal to
More informationDAMPING CONTROL OF A PZT MULTILAYER VIBRATION USING NEGATIVE IMPEDANCE CIRCUIT
International Workshop SMART MATERIALS, STRUCTURES & NDT in AEROSPACE Conference NDT in Canada 2011 2-4 November 2011, Montreal, Quebec, Canada DAMPING CONTROL OF A PZT MULTILAYER VIBRATION USING NEGATIVE
More informationMETHODS OF THEORETICAL PHYSICS
METHODS OF THEORETICAL PHYSICS Philip M. Morse PROFESSOR OF PHYSICS MASSACHUSETTS INSTITUTE OF TECHNOLOGY Herman Feshbach PROFESSOR OF PHYSICS MASSACHUSETTS INSTITUTE OF TECHNOLOGY PART II: CHAPTERS 9
More informationAdvanced Analog Building Blocks. Prof. Dr. Peter Fischer, Dr. Wei Shen, Dr. Albert Comerma, Dr. Johannes Schemmel, etc
Advanced Analog Building Blocks Prof. Dr. Peter Fischer, Dr. Wei Shen, Dr. Albert Comerma, Dr. Johannes Schemmel, etc 1 Topics 1. S domain and Laplace Transform Zeros and Poles 2. Basic and Advanced current
More informationActive Matter Lectures for the 2011 ICTP School on Mathematics and Physics of Soft and Biological Matter Lecture 3: Hydrodynamics of SP Hard Rods
Active Matter Lectures for the 2011 ICTP School on Mathematics and Physics of Soft and Biological Matter Lecture 3: of SP Hard Rods M. Cristina Marchetti Syracuse University Baskaran & MCM, PRE 77 (2008);
More informationConventional Paper I (a) (i) What are ferroelectric materials? What advantages do they have over conventional dielectric materials?
Conventional Paper I-03.(a) (i) What are ferroelectric materials? What advantages do they have over conventional dielectric materials? (ii) Give one example each of a dielectric and a ferroelectric material
More information16.584: Random (Stochastic) Processes
1 16.584: Random (Stochastic) Processes X(t): X : RV : Continuous function of the independent variable t (time, space etc.) Random process : Collection of X(t, ζ) : Indexed on another independent variable
More informationAnnouncements: Today: more AC circuits
Announcements: Today: more AC circuits I 0 I rms Current through a light bulb I 0 I rms I t = I 0 cos ωt I 0 Current through a LED I t = I 0 cos ωt Θ(cos ωt ) Theta function (is zero for a negative argument)
More information