Stochastic Structural Dynamics. Lecture-6

Similar documents
Stochastic Structural Dynamics. Lecture-12

5. Stochastic processes (1)

Elements of Stochastic Processes Lecture II Hamid R. Rabiee

Instructor: Dr. Heba A. Shaban Lecture # 4

Sensors, Signals and Noise

Anno accademico 2006/2007. Davide Migliore

Transform Techniques. Moment Generating Function

Lecture Notes 2. The Hilbert Space Approach to Time Series

Random Processes 1/24

LECTURE 1: GENERALIZED RAY KNIGHT THEOREM FOR FINITE MARKOV CHAINS

Physics 127b: Statistical Mechanics. Fokker-Planck Equation. Time Evolution

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

MODULE 3 FUNCTION OF A RANDOM VARIABLE AND ITS DISTRIBUTION LECTURES PROBABILITY DISTRIBUTION OF A FUNCTION OF A RANDOM VARIABLE

5. Response of Linear Time-Invariant Systems to Random Inputs

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ordinary Differential Equations

Vehicle Arrival Models : Headway

The consumption-based determinants of the term structure of discount rates: Corrigendum. Christian Gollier 1 Toulouse School of Economics March 2012

OBJECTIVES OF TIME SERIES ANALYSIS

Structural Dynamics and Earthquake Engineering

An Introduction to Malliavin calculus and its applications

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Diebold, Chapter 7. Francis X. Diebold, Elements of Forecasting, 4th Edition (Mason, Ohio: Cengage Learning, 2006). Chapter 7. Characterizing Cycles

(1) (2) Differentiation of (1) and then substitution of (3) leads to. Therefore, we will simply consider the second-order linear system given by (4)

Finite element method for structural dynamic and stability analyses

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

Application of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing

From Particles to Rigid Bodies

IB Physics Kinematics Worksheet

Chapter 1 Fundamental Concepts

International Journal of Scientific & Engineering Research, Volume 4, Issue 10, October ISSN

The Quantum Theory of Atoms and Molecules: The Schrodinger equation. Hilary Term 2008 Dr Grant Ritchie

Cash Flow Valuation Mode Lin Discrete Time

where the coordinate X (t) describes the system motion. X has its origin at the system static equilibrium position (SEP).

Zürich. ETH Master Course: L Autonomous Mobile Robots Localization II

The Strong Law of Large Numbers

Avd. Matematisk statistik

Mixing times and hitting times: lecture notes

14 Autoregressive Moving Average Models

m = 41 members n = 27 (nonfounders), f = 14 (founders) 8 markers from chromosome 19

Stochastic Processes. A. Bassi. RMP 85, April-June Appendix

L07. KALMAN FILTERING FOR NON-LINEAR SYSTEMS. NA568 Mobile Robotics: Methods & Algorithms

A quantum method to test the existence of consciousness

Filtering Turbulent Signals Using Gaussian and non-gaussian Filters with Model Error

Some Basic Information about M-S-D Systems

U( θ, θ), U(θ 1/2, θ + 1/2) and Cauchy (θ) are not exponential families. (The proofs are not easy and require measure theory. See the references.

On Multicomponent System Reliability with Microshocks - Microdamages Type of Components Interaction

15. Vector Valued Functions

Program: RFEM 5, RSTAB 8, RF-DYNAM Pro, DYNAM Pro. Category: Isotropic Linear Elasticity, Dynamics, Member

2.3 SCHRÖDINGER AND HEISENBERG REPRESENTATIONS

6. Stochastic calculus with jump processes

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

arxiv: v1 [math.pr] 19 Feb 2011

Institute for Mathematical Methods in Economics. University of Technology Vienna. Singapore, May Manfred Deistler

Undetermined coefficients for local fractional differential equations

Overview. COMP14112: Artificial Intelligence Fundamentals. Lecture 0 Very Brief Overview. Structure of this course

The motions of the celt on a horizontal plane with viscous friction

EE 315 Notes. Gürdal Arslan CLASS 1. (Sections ) What is a signal?

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

4.5 Constant Acceleration

Foundations of Statistical Inference. Sufficient statistics. Definition (Sufficiency) Definition (Sufficiency)

Non-uniform circular motion *

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

4.6 One Dimensional Kinematics and Integration

Reliability of Technical Systems

Basic notions of probability theory (Part 2)

Hamilton- J acobi Equation: Explicit Formulas In this lecture we try to apply the method of characteristics to the Hamilton-Jacobi equation: u t

ψ(t) = V x (0)V x (t)

Motion along a Straight Line

Nature Neuroscience: doi: /nn Supplementary Figure 1. Spike-count autocorrelations in time.

Let us start with a two dimensional case. We consider a vector ( x,

0 time. 2 Which graph represents the motion of a car that is travelling along a straight road with a uniformly increasing speed?

Linear Response Theory: The connection between QFT and experiments

Discrete Markov Processes. 1. Introduction

Chapter 15 Oscillatory Motion I

2.1: What is physics? Ch02: Motion along a straight line. 2.2: Motion. 2.3: Position, Displacement, Distance

Block Diagram of a DCS in 411

Two Coupled Oscillators / Normal Modes

A generalization of the Burg s algorithm to periodically correlated time series

Finish reading Chapter 2 of Spivak, rereading earlier sections as necessary. handout and fill in some missing details!

non -negative cone Population dynamics motivates the study of linear models whose coefficient matrices are non-negative or positive.

Calculus and Seismic Analysis November Ken Mark Bechtel Project Manager

The expectation value of the field operator.

KINEMATICS IN ONE DIMENSION

Finite element method for structural dynamic and stability analyses

An random variable is a quantity that assumes different values with certain probabilities.

Notes on Kalman Filtering

( ) ( ) if t = t. It must satisfy the identity. So, bulkiness of the unit impulse (hyper)function is equal to 1. The defining characteristic is

Unit Root Time Series. Univariate random walk

Homework sheet Exercises done during the lecture of March 12, 2014

Exam #3 Review. Skills #6 21.3, 24.2, 24.6, 25.1

BEng (Hons) Telecommunications. Examinations for / Semester 2

k 1 k 2 x (1) x 2 = k 1 x 1 = k 2 k 1 +k 2 x (2) x k series x (3) k 2 x 2 = k 1 k 2 = k 1+k 2 = 1 k k 2 k series

Martingales Stopping Time Processes

Lecture 10: The Poincaré Inequality in Euclidean space

Random variables. A random variable X is a function that assigns a real number, X(ζ), to each outcome ζ in the sample space of a random experiment.

Lecture 4 Kinetics of a particle Part 3: Impulse and Momentum

Phys 221 Fall Chapter 2. Motion in One Dimension. 2014, 2005 A. Dzyubenko Brooks/Cole

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

Transcription:

Sochasic Srucural Dynamics Lecure-6 Random processes- Dr C S Manohar Deparmen of Civil Engineering Professor of Srucural Engineering Indian Insiue of Science Bangalore 560 0 India manohar@civil.iisc.erne.in

Review of heory of Random processes

Guideway unevenness d mu c u yv k u yv 0 d d mu cu ku c yvk yv f () d For eample if y ( ) sin f cvcos v ksin v. For more complicaed forms of guideway uneveness f( ) would be more complicaed. 3

Sae Noion of a random process Ensemble Parameer (ime) Working definiion: A random variable ha evolves in ime. Or Parameered family of random variables. 4

Analogy Random variable Saics Random process Dynamics When o model a quaniy as random variable and when o model i as a random process? This is analogous o asking when o model a sysem as saic and when as dynamic. 5

Recall Random variable is a funcion from sample space ino real line such ha () for every R : X( ) is an even () P : X( ) 0 A random process is a funcion: RR and is denoed by X and is wrien as X( ) such ha ( a)for a fied value of X is a random variable (b) for a fied value of X is a funcion of ime (a realizaion) (c) for fied values of and X is a number and (d) for varying and X is collecion of ime hisories (ensemble). 6

Terminology Evoluion in ime : Random processes Evoluion in space: Random fields Mahemaically i is no necessary o mainain his disincion Sochasic processes Sochasic field Random funcions Time series 7

A scheme for classificaion of random processes Le X be a random process. =parameer; values aken by X =sae. For fied value of X If X is a discree random variable hen is a random process wih a discree sae space. X If X is a coninuous random variable hen is a random process wih a coninuous sae space. If akes only discree values we say ha X is a random process wih discree paramers. If akes coninuous values we say ha X is a random process wih coninuous parameers. 8

Four caegories of random processes (a) discree sae discree parameer random processes (b) discree sae coninuous parameer random processes (a) coninuous sae discree parameer random processes (a) coninuous sae coninuous parameer random processes 9

Parameer need no always be ime Evoluion of wind velociy in space and ime Oher eamples (a) Road roughness (evoluion in space) (b) wave heighs (evoluion in space and ime) (c) Thickness of a cylindrical shell (evoluion in an angle) (d) FRF-s evoluion in frequency (and space) 0

z y fied d () Vecor random process u g d () vg : ground displacemen w g u g v ( ) v g : ground velociy w g u g a () vg : ground accelearion w g

Descripion of a random process Firs order Probabiliy Disribuion Funcion ; PX P X Firs order probabiliy densiy funcion p X ; PX ; Random variable PX ; Sae variable Parameer

3 ; Second order Probabiliy Disribuion Funcion X X P P XX ; ; Second order probabiliy densiy funcion P p XX XX

4 h order Probabiliy Disribuion Funcion ; n i i X i n- P P X n X n X P p n ~ ~ ~ ~ ; ~ ~ ; h order probabiliy densiy funcion -

Complee descripion of a random process Specify P ~ X ~ ~ ; for all n and for any choice of ~. OR Specify p ~ X ~ ~ ; for all n and for any choice of. ~ 5

Epecaion of a random process Mean Variance 6

Auocovariance Auocorrelaion Auocorrelaion coefficien 7

Remarks (a) C R if m m 0 XX XX X X X C (b) XX (c) r (prove i) XX 8

Gaussian random process Le X( ) be a random process and consider is s and nd order pdf-s. mx px ; ep ; X X pxx ; r ep r m m m m r ; ; ; ; m m m m r r X X X X XX 9

i i Coninuing furher consider n ime insans and associaed random variables X. Le he jpdf of X be given by i n pxxx n; n ep ; n i S S i n n i S i n X m X m ij i X i j X j Noe : S S & S is posiive definie. m m m X X X n X Definiion n is said o be a Gaussian random process if he above form of pdf is rue for any n and for any choice of. i n i i 0

Saionariy of a random process Analogous o concep of seady sae in vibraion problems One or more of he properies of random process becomes independen of ime Srong sense saionariy (SSS) : defined wih respec o pdf-s Wide sense saionariy (WSS) : defined wih respec o momens

s order nd order n-h order SSS 3

n i i n n X XX n n X XX n p p X & ; ; )is said o be SSS ( h order SSS. - is hen we say ha values of and no for all rue only for he above resul is If m X() n m n

Remark (a) Wha happen o mean and variance of a s order SSS process? 5

Remark (b) Eercise Show ha nd order SSS implies s order SSS 6

Remark (c) Wha happens o covariance of a nd order SSS process? 7

Remark (d) X m C X XX is said o be nd order WSSif is independen of C XX ime and 8

Remarks (Coninued) (e) The defaul noion of saionariy is nd order WSS. (f) For a process ha is evolving in space he erm homogeneiy is used o denoe saionariy. (g) A process ha is no saionary is called nonsaionary. (h) Noion of join saionariy of wo or more random processes can also be defined. 9

Wind velociy: Saionary in ime Nonsaionary in space 30

Earhquake ground acceleraion Acceleraion ime 3

Ergodicy of a random process Basic noion Equivalence of emporal and ensemble averages Ensemble Direcion Temporal Direcion 3

33

5/3/0 34

5/3/0 35

Ergodiciy in mean Le X() be a saionary random process wih specified join pdf srucure T T T T 0 T T X() d is a random variable T ET E[ X( )] d E( ) T T T T E X ( ) X ( ) d d T 4T T T [ R( ) ] d T T 36