Math 597/697: Solution 5
|
|
- Karin Betty Sutton
- 5 years ago
- Views:
Transcription
1 Math 597/697: Solution 5 The transition between the the ifferent states is governe by the transition matrix P = 4 0 5, () an v 0 = /4, v = 5, v 2 = /3, v 3 = /5 Hence the generator is given by (2) 2 The state space consists of all pairs (m, n) of nonnegative integers The time until a given pair of male an female prouces an offspring is an exponential RV with parameter λ If the population at time consists of m males an n females there are nm possible pairs an hence we obtain v (m,n) = λmn, (3) q (m,n)(m+,n) = pλmn, q (m,n)(m,n+) = ( p)λmn (4) P (m,n)(m+,n) = p, P (m,n)(m,n+) = ( p) (5) 3 (a) The number of computers X t in operating conition at time t is either 0,, 2 an the number of computers operating is either 0 if X t = 0 or if X t = or 2 The rate of failure of the operating computer is an the rate of repair is λ There is only one repair facility so that at most one computer can be repaire at a time We fin an v 0 = λ, v = λ +, v 2 = (6) P 0 =, P 0 = λ +, P 2 = λ λ +, P 2 = (7)
2 Hence the generator is λ λ 0 λ λ 0 The backwar equations are, for j = 0,, 2, (8) t P 0j = λ(p 0j P j ), (9) t P j = (P 0j P j ) λ(p j P 2j ), (0) t P 2j = (P j P 2j ), () an the forwar equations are t P j0 = λp j0 + P j, (2) t P j = λp j0 (λ + )P j + P j2, (3) t P j2 = λp j P j2 (4) The stationary istribution is π j = (λ/) j + (λ/) + (λ/) 2 (5) It is also a limiting istribution since the state space is finite an the chain is irreucible In the long run, the proportion of time when the system is operating (ie in state or 2) is (λ/) + (λ/) 2 + (λ/) + (λ/) 2 (6) (b) The ifference with (a) is that the two computers can be in operation at the same time an so the rate of failures when X t = 2 is twice the rate of (a) v 0 = λ, v = λ +, v 2 = 2 (7) Then λ λ 0 λ λ 0 2 2, (8) 2
3 an the stationary istribution is in that case π j = j! (λ/)j + (λ/) + 2 (λ/)2 (9) an so, in the long run, the proportion of time when the system is operating (ie in state or 2) is (λ/) + 2 (λ/)2 + (λ/) + 2 (λ/)2 (20) (c) Let us consier first the case (a) We compute the expecte time to reach 0 starting from 2 We write T = T 2 + T 0 where T 2 is the first time the chain reach state stating from state 2 an T 0 is the first time the chain reach state 0 starting from Clearly T 2 is an exponential RV with mean To compute E[T 0] we conition on the event A where the first transition is to 0 (probability /(λ + ) or the event B where the first transition is to 2 (probability λ/(λ + ) Since the first transition occurs in average after a time /(λ + ) we fin E[T 0 A] = E[T 0 B] = λ +, (2) λ + + E[T 2] + E[T 0 ] (22) an so, E[T 0 ] = = λ + + λ + ( + λ ) + λ λ + (E[T 2] + E[T 0 ]) (23) λ λ + E[T 0]) (24) Solving gives E[T 0 ] = + λ an E[T ] = 2+ λ In case (b) one fins λ 2 instea 4 Each component is an on/off system with generator ( λi λ i i i ) (25) 3
4 For each component the stationary an limiting istribution is for i = A, B, π (i) i 0 =, π (i) λ i = (26) λ i + i λ i + i By inepenence the stationary istribution of the two componentsystem is π (A) i π (B) j (a) If the components are working in parallel the is operating if at least of the components is in state 0, hence the esire probability is π (A) π (B) = λ A λ B (λ A + A )(λ B + B ) (27) (b) If the components are working in series, both must work for the system to be operating, hence the esire probability is π (A) 0 π (B) 0 = A B (λ A + A )(λ B + B ) (28) 5 Consier a continuous time branching process efine as follows A organism lifetime is exponential with parameter λ an upon eath, it leaves k offspring with probability p k, k 0 The organisms act inepenently of each other We assume that p = 0 so that, at eath, there are no transition from a state into itself Let X t be the population at time t A transition occurs when an organism ies an if there are n organisms the average time until a eath is /nλ an so v n = nλ When an organism ies it is replace by 0, 2, 3, 4, organisms an therefore we have P nn = p 0 P nn+ = p 2, P nn+k = p k+ (29) Therefore the generator is given by λp 0 λ λp 2 λp 3 0 2λp 0 2λ 2λp 2 (30) The backwar equations are t P 0j = 0, (3) 4
5 t P j = λ (p 0 P 0j + p 2 P 2j + p 3 P 3j + P j ), (32) (33) t P nj = nλ (p 0 P n j + p 2 P n+j + p 3 P n+2j + P nj ) (34) an the forwar equations are t P j0 = λp 0 P j, (35) t P j = λp j + 2λp 0 P j2, (36) t P j2 = λp 2 P j + 2λP j2 + 3λp 0 P j3, (37) t P j3 = λp 3 P j + 2λp 2 P j2 3λP j3 + 4λp 0 λp j3, (38) (39) In case of binary splitting we have if the probability of eath without offspring is p λp λ λ( p) 0 0 2λp 2λ 2λ( p) (40) As ones sees from the matrix A the Markov chain is not irreucible, 0 is an absorbing state an all other states are transient The istribution π = (, 0, 0, 0, ) is a stationary state, which escribe the situation where noboy lives Note that the transition matrix P ij is given by a ranom walk, so one might expect that if p < /2 every initial istribution will converge to π while if p /2 there will be a positive probability to escape to infinity 6 Consier the M/M/ queue with arrival rate λ an service rate (a) The M/M/ queue is a Birth an Death process with λ n = λ 5
6 an n = n Hence the generator is λ λ λ λ λ 2 λ λ 3 λ (4) (b) Using the general solution for the stationary an limiting istribution for a Birth an Death process (the M/M/ is irreucible) one fins λ n λ 0 λ n + = + n= n n! n= n = e(λ/) (42) an so ) n e (λ/) (43) π n = n! ( λ The M/M/ is positive recurrent an the stationary istribution is Poisson with parameter λ/ (c) Since we have P {X t+h = n + X t = n} = λh + o(h), (44) P {X t+h = n X t = n} = nh + o(h), (45) P {X t+h = n X t = n} = ( λh nh) + o(h),(46) E [X t+h X t = n] (47) = (n + )λh + (n )nh + n( λh nh) + o(h),(48) = λh nh + n + o(h) (49) an Therefore an E [X t+h ] = λh he [X t ] + E [X t ] + o(h) (50) t E [X t] = λ E [X t ] (5) E [X t ] = E [X 0 ] e t + λ ( e t) (52) 6
7 7 Consier a queuing system with one single server, arrival rate λ an serving rate (a) When N customers are in the system, the arriving customers give up an o no enter the system So the state space is {0,,, N}, the generator is λ λ 0 0 λ λ 0 0 (53) 0 0 λ λ 0 0 The limiting istribution can be foun using the general formula for the birth an eath process with λ n = 0 for n N One fins for 0 j N π j = (λ/) j + N k= (λ/) k = (λ/) j ( (λ/)) λ (λ/) N+ N+ λ = (54) (b) When n customers are in the system, an arriving customer will join the system with probability /(n + ) We have n = for n an λ n = λ/(n + ) for 0n 0 Then λ n λ 0 λ n + = + n= n n! n= n = e(λ/) (55) an the stationary istribution is Poisson with parameter λ/ 8 Consier a Yule process (pure birth with linear growth) an let T i be the time it takes for a population of size i to reach i + (a) Since it is a pure birth process T i is exponential with rate iλ (b) Let us suppose we have n components with ii exponential lifetime X i The RV max(x,, X n ) is the time it takes for the n components to fail Starting with n components, the time until the first failure is the minimum of n exponential RV with parameter λ which is an exponential RV T n with parameter nλ By the memoryless property of the exponential, the time between the first failure an the secon failure is, again, the minimum of 7
8 n exponential RV with parameter λ which is is an exponential RV T n with parameter (n )λ Hence max(x,, X n ) = T n + T n + + T (56) (c) We have, by (b), an inepenence P {T + T 2 + T n < t} = P {max(x,, X n ) < t} = P {X < t} P {X n < t} = ( e λt ) n (57) () Since X t is a pure birth process the Markov chain X t only makes transition from j to j + So T + +T n is the time necessary to reach n starting from an P {T + + T n < t} is the probability that X t n P n (t) = P {X t = n X 0 = } = P {X t n X 0 = } P {X t n + X 0 = } = P {T + + T n < t} P {T + + T n < t} = ( e λt ) n ( e λt ) n = e λt ( e λt ) n (58) Hence P {X t = n X 0 = } has a geometric istribution with parameter e λt (e) By () X t conitione on {X 0 = } is a geometric ranom variable By efinition of a Birth process, the iniviuals reprouce inepenently of each other, an therefore X t conitione on {X 0 = m} is the sum of m geometric ranom variables The sum of m geometric RV with parameters p is calle a negative binomial RV with parameters (m, p) A geometric RV is the number of inepenent trials necessary to obtain one success, so that a negative binomial RV is the number of trials necessary to obtain exactly m successes The probability istribution of the negative binomial RV is, for k m, (at least m trials are necessary) p(k) = ( ) k p m ( p) k m (59) m 8
9 The combinatorial factor is obtaine by noting that the last trial must be a success an by counting the number of ways of having the remaining m successes Therefore we obtain, for n m ( ) n P mn (t) = (e λt ) m ( e λt ) n m (60) m 9
Continuous-Time Markov Chain
Continuous-Time Markov Chain Consider the process {X(t),t 0} with state space {0, 1, 2,...}. The process {X(t),t 0} is a continuous-time Markov chain if for all s, t 0 and nonnegative integers i, j, x(u),
More informationMarkov Chains. X(t) is a Markov Process if, for arbitrary times t 1 < t 2 <... < t k < t k+1. If X(t) is discrete-valued. If X(t) is continuous-valued
Markov Chains X(t) is a Markov Process if, for arbitrary times t 1 < t 2
More informationMATH 56A: STOCHASTIC PROCESSES CHAPTER 3
MATH 56A: STOCHASTIC PROCESSES CHAPTER 3 Plan for rest of semester (1) st week (8/31, 9/6, 9/7) Chap 0: Diff eq s an linear recursion (2) n week (9/11...) Chap 1: Finite Markov chains (3) r week (9/18...)
More informationSTAT 380 Continuous Time Markov Chains
STAT 380 Continuous Time Markov Chains Richard Lockhart Simon Fraser University Spring 2018 Richard Lockhart (Simon Fraser University)STAT 380 Continuous Time Markov Chains Spring 2018 1 / 35 Continuous
More informationChapter 5. Continuous-Time Markov Chains. Prof. Shun-Ren Yang Department of Computer Science, National Tsing Hua University, Taiwan
Chapter 5. Continuous-Time Markov Chains Prof. Shun-Ren Yang Department of Computer Science, National Tsing Hua University, Taiwan Continuous-Time Markov Chains Consider a continuous-time stochastic process
More informationReadings: Finish Section 5.2
LECTURE 19 Readings: Finish Section 5.2 Lecture outline Markov Processes I Checkout counter example. Markov process: definition. -step transition probabilities. Classification of states. Example: Checkout
More informationStatistics 150: Spring 2007
Statistics 150: Spring 2007 April 23, 2008 0-1 1 Limiting Probabilities If the discrete-time Markov chain with transition probabilities p ij is irreducible and positive recurrent; then the limiting probabilities
More informationThe Transition Probability Function P ij (t)
The Transition Probability Function P ij (t) Consider a continuous time Markov chain {X(t), t 0}. We are interested in the probability that in t time units the process will be in state j, given that it
More informationProbability and Statistics Concepts
University of Central Florida Computer Science Division COT 5611 - Operating Systems. Spring 014 - dcm Probability and Statistics Concepts Random Variable: a rule that assigns a numerical value to each
More informationContinuous Time Markov Chains
Continuous Time Markov Chains Stochastic Processes - Lecture Notes Fatih Cavdur to accompany Introduction to Probability Models by Sheldon M. Ross Fall 2015 Outline Introduction Continuous-Time Markov
More informationIntroduction to Queuing Networks Solutions to Problem Sheet 3
Introduction to Queuing Networks Solutions to Problem Sheet 3 1. (a) The state space is the whole numbers {, 1, 2,...}. The transition rates are q i,i+1 λ for all i and q i, for all i 1 since, when a bus
More informationλ λ λ In-class problems
In-class problems 1. Customers arrive at a single-service facility at a Poisson rate of 40 per hour. When two or fewer customers are present, a single attendant operates the facility, and the service time
More informationLECTURE #6 BIRTH-DEATH PROCESS
LECTURE #6 BIRTH-DEATH PROCESS 204528 Queueing Theory and Applications in Networks Assoc. Prof., Ph.D. (รศ.ดร. อน นต ผลเพ ม) Computer Engineering Department, Kasetsart University Outline 2 Birth-Death
More information57:022 Principles of Design II Final Exam Solutions - Spring 1997
57:022 Principles of Design II Final Exam Solutions - Spring 1997 Part: I II III IV V VI Total Possible Pts: 52 10 12 16 13 12 115 PART ONE Indicate "+" if True and "o" if False: + a. If a component's
More informationContinuous time Markov chains
Continuous time Markov chains Alejandro Ribeiro Dept. of Electrical and Systems Engineering University of Pennsylvania aribeiro@seas.upenn.edu http://www.seas.upenn.edu/users/~aribeiro/ October 16, 2017
More informationStochastic process. X, a series of random variables indexed by t
Stochastic process X, a series of random variables indexed by t X={X(t), t 0} is a continuous time stochastic process X={X(t), t=0,1, } is a discrete time stochastic process X(t) is the state at time t,
More informationThe exponential distribution and the Poisson process
The exponential distribution and the Poisson process 1-1 Exponential Distribution: Basic Facts PDF f(t) = { λe λt, t 0 0, t < 0 CDF Pr{T t) = 0 t λe λu du = 1 e λt (t 0) Mean E[T] = 1 λ Variance Var[T]
More informationCDA5530: Performance Models of Computers and Networks. Chapter 3: Review of Practical
CDA5530: Performance Models of Computers and Networks Chapter 3: Review of Practical Stochastic Processes Definition Stochastic ti process X = {X(t), t T} is a collection of random variables (rvs); one
More informationIEOR 6711, HMWK 5, Professor Sigman
IEOR 6711, HMWK 5, Professor Sigman 1. Semi-Markov processes: Consider an irreducible positive recurrent discrete-time Markov chain {X n } with transition matrix P (P i,j ), i, j S, and finite state space.
More informationContinuous-time Markov Chains
Continuous-time Markov Chains Gonzalo Mateos Dept. of ECE and Goergen Institute for Data Science University of Rochester gmateosb@ece.rochester.edu http://www.ece.rochester.edu/~gmateosb/ October 23, 2017
More informationEXAM IN COURSE TMA4265 STOCHASTIC PROCESSES Wednesday 7. August, 2013 Time: 9:00 13:00
Norges teknisk naturvitenskapelige universitet Institutt for matematiske fag Page 1 of 7 English Contact: Håkon Tjelmeland 48 22 18 96 EXAM IN COURSE TMA4265 STOCHASTIC PROCESSES Wednesday 7. August, 2013
More informationAn M/G/1 Retrial Queue with Priority, Balking and Feedback Customers
Journal of Convergence Information Technology Volume 5 Number April 1 An M/G/1 Retrial Queue with Priority Balking an Feeback Customers Peishu Chen * 1 Yiuan Zhu 1 * 1 Faculty of Science Jiangsu University
More informationRecap. Probability, stochastic processes, Markov chains. ELEC-C7210 Modeling and analysis of communication networks
Recap Probability, stochastic processes, Markov chains ELEC-C7210 Modeling and analysis of communication networks 1 Recap: Probability theory important distributions Discrete distributions Geometric distribution
More informationSolutions to Homework Discrete Stochastic Processes MIT, Spring 2011
Exercise 6.5: Solutions to Homework 0 6.262 Discrete Stochastic Processes MIT, Spring 20 Consider the Markov process illustrated below. The transitions are labelled by the rate q ij at which those transitions
More informationTMA4265 Stochastic processes ST2101 Stochastic simulation and modelling
Norwegian University of Science and Technology Department of Mathematical Sciences Page of 7 English Contact during examination: Øyvind Bakke Telephone: 73 9 8 26, 99 4 673 TMA426 Stochastic processes
More informationOutline. Finite source queue M/M/c//K Queues with impatience (balking, reneging, jockeying, retrial) Transient behavior Advanced Queue.
Outline Finite source queue M/M/c//K Queues with impatience (balking, reneging, jockeying, retrial) Transient behavior Advanced Queue Batch queue Bulk input queue M [X] /M/1 Bulk service queue M/M [Y]
More informationIrreducibility. Irreducible. every state can be reached from every other state For any i,j, exist an m 0, such that. Absorbing state: p jj =1
Irreducibility Irreducible every state can be reached from every other state For any i,j, exist an m 0, such that i,j are communicate, if the above condition is valid Irreducible: all states are communicate
More informationBulk input queue M [X] /M/1 Bulk service queue M/M [Y] /1 Erlangian queue M/E k /1
Advanced Markovian queues Bulk input queue M [X] /M/ Bulk service queue M/M [Y] / Erlangian queue M/E k / Bulk input queue M [X] /M/ Batch arrival, Poisson process, arrival rate λ number of customers in
More informationECE-517: Reinforcement Learning in Artificial Intelligence. Lecture 4: Discrete-Time Markov Chains
ECE-517: Reinforcement Learning in Artificial Intelligence Lecture 4: Discrete-Time Markov Chains September 1, 215 Dr. Itamar Arel College of Engineering Department of Electrical Engineering & Computer
More information(b) What is the variance of the time until the second customer arrives, starting empty, assuming that we measure time in minutes?
IEOR 3106: Introduction to Operations Research: Stochastic Models Fall 2006, Professor Whitt SOLUTIONS to Final Exam Chapters 4-7 and 10 in Ross, Tuesday, December 19, 4:10pm-7:00pm Open Book: but only
More informationIntroduction to queuing theory
Introduction to queuing theory Queu(e)ing theory Queu(e)ing theory is the branch of mathematics devoted to how objects (packets in a network, people in a bank, processes in a CPU etc etc) join and leave
More informationSTATS 3U03. Sang Woo Park. March 29, Textbook: Inroduction to stochastic processes. Requirement: 5 assignments, 2 tests, and 1 final
STATS 3U03 Sang Woo Park March 29, 2017 Course Outline Textbook: Inroduction to stochastic processes Requirement: 5 assignments, 2 tests, and 1 final Test 1: Friday, February 10th Test 2: Friday, March
More informationPart I Stochastic variables and Markov chains
Part I Stochastic variables and Markov chains Random variables describe the behaviour of a phenomenon independent of any specific sample space Distribution function (cdf, cumulative distribution function)
More informationMarkov Chains in Continuous Time
Chapter 23 Markov Chains in Continuous Time Previously we looke at Markov chains, where the transitions betweenstatesoccurreatspecifietime- steps. That it, we mae time (a continuous variable) avance in
More informationreversed chain is ergodic and has the same equilibrium probabilities (check that π j =
Lecture 10 Networks of queues In this lecture we shall finally get around to consider what happens when queues are part of networks (which, after all, is the topic of the course). Firstly we shall need
More informationEE126: Probability and Random Processes
EE126: Probability and Random Processes Lecture 19: Poisson Process Abhay Parekh UC Berkeley March 31, 2011 1 1 Logistics 2 Review 3 Poisson Processes 2 Logistics 3 Poisson Process A continuous version
More informationComputer Systems Modelling
Computer Systems Modelling Computer Laboratory Computer Science Tripos, Part II Lent Term 2010/11 R. J. Gibbens Problem sheet William Gates Building 15 JJ Thomson Avenue Cambridge CB3 0FD http://www.cl.cam.ac.uk/
More informationFigure 10.1: Recording when the event E occurs
10 Poisson Processes Let T R be an interval. A family of random variables {X(t) ; t T} is called a continuous time stochastic process. We often consider T = [0, 1] and T = [0, ). As X(t) is a random variable
More informationLecturer: Olga Galinina
Renewal models Lecturer: Olga Galinina E-mail: olga.galinina@tut.fi Outline Reminder. Exponential models definition of renewal processes exponential interval distribution Erlang distribution hyperexponential
More informationAn Introduction to Stochastic Modeling
F An Introduction to Stochastic Modeling Fourth Edition Mark A. Pinsky Department of Mathematics Northwestern University Evanston, Illinois Samuel Karlin Department of Mathematics Stanford University Stanford,
More informationName of the Student:
SUBJECT NAME : Probability & Queueing Theory SUBJECT CODE : MA 6453 MATERIAL NAME : Part A questions REGULATION : R2013 UPDATED ON : November 2017 (Upto N/D 2017 QP) (Scan the above QR code for the direct
More informationMARKOV PROCESSES. Valerio Di Valerio
MARKOV PROCESSES Valerio Di Valerio Stochastic Process Definition: a stochastic process is a collection of random variables {X(t)} indexed by time t T Each X(t) X is a random variable that satisfy some
More informationMarkov Model. Model representing the different resident states of a system, and the transitions between the different states
Markov Model Model representing the different resident states of a system, and the transitions between the different states (applicable to repairable, as well as non-repairable systems) System behavior
More information2. Transience and Recurrence
Virtual Laboratories > 15. Markov Chains > 1 2 3 4 5 6 7 8 9 10 11 12 2. Transience and Recurrence The study of Markov chains, particularly the limiting behavior, depends critically on the random times
More information1 Math 285 Homework Problem List for S2016
1 Math 85 Homework Problem List for S016 Note: solutions to Lawler Problems will appear after all of the Lecture Note Solutions. 1.1 Homework 1. Due Friay, April 8, 016 Look at from lecture note exercises:
More informationCDA6530: Performance Models of Computers and Networks. Chapter 3: Review of Practical Stochastic Processes
CDA6530: Performance Models of Computers and Networks Chapter 3: Review of Practical Stochastic Processes Definition Stochastic process X = {X(t), t2 T} is a collection of random variables (rvs); one rv
More informationSTA 624 Practice Exam 2 Applied Stochastic Processes Spring, 2008
Name STA 624 Practice Exam 2 Applied Stochastic Processes Spring, 2008 There are five questions on this test. DO use calculators if you need them. And then a miracle occurs is not a valid answer. There
More informationQueueing Theory I Summary! Little s Law! Queueing System Notation! Stationary Analysis of Elementary Queueing Systems " M/M/1 " M/M/m " M/M/1/K "
Queueing Theory I Summary Little s Law Queueing System Notation Stationary Analysis of Elementary Queueing Systems " M/M/1 " M/M/m " M/M/1/K " Little s Law a(t): the process that counts the number of arrivals
More informationExamples of Countable State Markov Chains Thursday, October 16, :12 PM
stochnotes101608 Page 1 Examples of Countable State Markov Chains Thursday, October 16, 2008 12:12 PM Homework 2 solutions will be posted later today. A couple of quick examples. Queueing model (without
More informationLecture 4a: Continuous-Time Markov Chain Models
Lecture 4a: Continuous-Time Markov Chain Models Continuous-time Markov chains are stochastic processes whose time is continuous, t [0, ), but the random variables are discrete. Prominent examples of continuous-time
More informationQueuing Theory. Richard Lockhart. Simon Fraser University. STAT 870 Summer 2011
Queuing Theory Richard Lockhart Simon Fraser University STAT 870 Summer 2011 Richard Lockhart (Simon Fraser University) Queuing Theory STAT 870 Summer 2011 1 / 15 Purposes of Today s Lecture Describe general
More information2905 Queueing Theory and Simulation PART III: HIGHER DIMENSIONAL AND NON-MARKOVIAN QUEUES
295 Queueing Theory and Simulation PART III: HIGHER DIMENSIONAL AND NON-MARKOVIAN QUEUES 16 Queueing Systems with Two Types of Customers In this section, we discuss queueing systems with two types of customers.
More informationHomework set 4 - Solutions
Homework set 4 - Solutions Math 495 Renato Feres Probability background for continuous time Markov chains This long introduction is in part about topics likely to have been covered in math 3200 or math
More informationStochastic Models in Computer Science A Tutorial
Stochastic Models in Computer Science A Tutorial Dr. Snehanshu Saha Department of Computer Science PESIT BSC, Bengaluru WCI 2015 - August 10 to August 13 1 Introduction 2 Random Variable 3 Introduction
More informationLecture 20: Reversible Processes and Queues
Lecture 20: Reversible Processes and Queues 1 Examples of reversible processes 11 Birth-death processes We define two non-negative sequences birth and death rates denoted by {λ n : n N 0 } and {µ n : n
More informationExercises Solutions. Automation IEA, LTH. Chapter 2 Manufacturing and process systems. Chapter 5 Discrete manufacturing problems
Exercises Solutions Note, that we have not formulated the answers for all the review questions. You will find the answers for many questions by reading and reflecting about the text in the book. Chapter
More informationMarkov chains. 1 Discrete time Markov chains. c A. J. Ganesh, University of Bristol, 2015
Markov chains c A. J. Ganesh, University of Bristol, 2015 1 Discrete time Markov chains Example: A drunkard is walking home from the pub. There are n lampposts between the pub and his home, at each of
More informationNOTES ON EULER-BOOLE SUMMATION (1) f (l 1) (n) f (l 1) (m) + ( 1)k 1 k! B k (y) f (k) (y) dy,
NOTES ON EULER-BOOLE SUMMATION JONATHAN M BORWEIN, NEIL J CALKIN, AND DANTE MANNA Abstract We stuy a connection between Euler-MacLaurin Summation an Boole Summation suggeste in an AMM note from 196, which
More informationContinuous-Valued Probability Review
CS 6323 Continuous-Valued Probability Review Prof. Gregory Provan Department of Computer Science University College Cork 2 Overview Review of discrete distributions Continuous distributions 3 Discrete
More information1 IEOR 4701: Continuous-Time Markov Chains
Copyright c 2006 by Karl Sigman 1 IEOR 4701: Continuous-Time Markov Chains A Markov chain in discrete time, {X n : n 0}, remains in any state for exactly one unit of time before making a transition (change
More informationConvergence of Random Walks
Chapter 16 Convergence of Ranom Walks This lecture examines the convergence of ranom walks to the Wiener process. This is very important both physically an statistically, an illustrates the utility of
More informationBirth-Death Processes
Birth-Death Processes Birth-Death Processes: Transient Solution Poisson Process: State Distribution Poisson Process: Inter-arrival Times Dr Conor McArdle EE414 - Birth-Death Processes 1/17 Birth-Death
More informationChapter 8 Queuing Theory Roanna Gee. W = average number of time a customer spends in the system.
8. Preliminaries L, L Q, W, W Q L = average number of customers in the system. L Q = average number of customers waiting in queue. W = average number of time a customer spends in the system. W Q = average
More informationLecture 21. David Aldous. 16 October David Aldous Lecture 21
Lecture 21 David Aldous 16 October 2015 In continuous time 0 t < we specify transition rates or informally P(X (t+δ)=j X (t)=i, past ) q ij = lim δ 0 δ P(X (t + dt) = j X (t) = i) = q ij dt but note these
More informationAnswers to selected exercises
Answers to selected exercises A First Course in Stochastic Models, Henk C. Tijms 1.1 ( ) 1.2 (a) Let waiting time if passengers already arrived,. Then,, (b) { (c) Long-run fraction for is (d) Let waiting
More informationTHE QUEEN S UNIVERSITY OF BELFAST
THE QUEEN S UNIVERSITY OF BELFAST 0SOR20 Level 2 Examination Statistics and Operational Research 20 Probability and Distribution Theory Wednesday 4 August 2002 2.30 pm 5.30 pm Examiners { Professor R M
More informationQueuing Theory. Using the Math. Management Science
Queuing Theory Using the Math 1 Markov Processes (Chains) A process consisting of a countable sequence of stages, that can be judged at each stage to fall into future states independent of how the process
More information3. Poisson Processes (12/09/12, see Adult and Baby Ross)
3. Poisson Processes (12/09/12, see Adult and Baby Ross) Exponential Distribution Poisson Processes Poisson and Exponential Relationship Generalizations 1 Exponential Distribution Definition: The continuous
More informationTMA 4265 Stochastic Processes
TMA 4265 Stochastic Processes Norges teknisk-naturvitenskapelige universitet Institutt for matematiske fag Solution - Exercise 9 Exercises from the text book 5.29 Kidney transplant T A exp( A ) T B exp(
More informationNetworking = Plumbing. Queueing Analysis: I. Last Lecture. Lecture Outline. Jeremiah Deng. 29 July 2013
Networking = Plumbing TELE302 Lecture 7 Queueing Analysis: I Jeremiah Deng University of Otago 29 July 2013 Jeremiah Deng (University of Otago) TELE302 Lecture 7 29 July 2013 1 / 33 Lecture Outline Jeremiah
More informationContinuous Time Processes
page 102 Chapter 7 Continuous Time Processes 7.1 Introduction In a continuous time stochastic process (with discrete state space), a change of state can occur at any time instant. The associated point
More informationPage 0 of 5 Final Examination Name. Closed book. 120 minutes. Cover page plus five pages of exam.
Final Examination Closed book. 120 minutes. Cover page plus five pages of exam. To receive full credit, show enough work to indicate your logic. Do not spend time calculating. You will receive full credit
More informationQUEUING MODELS AND MARKOV PROCESSES
QUEUING MODELS AND MARKOV ROCESSES Queues form when customer demand for a service cannot be met immediately. They occur because of fluctuations in demand levels so that models of queuing are intrinsically
More informationLecture Notes 7 Random Processes. Markov Processes Markov Chains. Random Processes
Lecture Notes 7 Random Processes Definition IID Processes Bernoulli Process Binomial Counting Process Interarrival Time Process Markov Processes Markov Chains Classification of States Steady State Probabilities
More informationAll models are wrong / inaccurate, but some are useful. George Box (Wikipedia). wkc/course/part2.pdf
PART II (3) Continuous Time Markov Chains : Theory and Examples -Pure Birth Process with Constant Rates -Pure Death Process -More on Birth-and-Death Process -Statistical Equilibrium (4) Introduction to
More informationMath Homework 5 Solutions
Math 45 - Homework 5 Solutions. Exercise.3., textbook. The stochastic matrix for the gambler problem has the following form, where the states are ordered as (,, 4, 6, 8, ): P = The corresponding diagram
More informationIntro Refresher Reversibility Open networks Closed networks Multiclass networks Other networks. Queuing Networks. Florence Perronnin
Queuing Networks Florence Perronnin Polytech Grenoble - UGA March 23, 27 F. Perronnin (UGA) Queuing Networks March 23, 27 / 46 Outline Introduction to Queuing Networks 2 Refresher: M/M/ queue 3 Reversibility
More informationT. Liggett Mathematics 171 Final Exam June 8, 2011
T. Liggett Mathematics 171 Final Exam June 8, 2011 1. The continuous time renewal chain X t has state space S = {0, 1, 2,...} and transition rates (i.e., Q matrix) given by q(n, n 1) = δ n and q(0, n)
More informationPromotion and Application of the M/M/1/N Queuing System
Mathematica Aeterna, Vol 2, 2012, no 7, 609-616 Promotion and Application of the M/M/1/N Queuing System Quanru Pan School of Mathematics and Physics, Jiangsu University of science and technology, Zhenjiang,
More informationLecture 7: Simulation of Markov Processes. Pasi Lassila Department of Communications and Networking
Lecture 7: Simulation of Markov Processes Pasi Lassila Department of Communications and Networking Contents Markov processes theory recap Elementary queuing models for data networks Simulation of Markov
More informationStochastic Processes. Theory for Applications. Robert G. Gallager CAMBRIDGE UNIVERSITY PRESS
Stochastic Processes Theory for Applications Robert G. Gallager CAMBRIDGE UNIVERSITY PRESS Contents Preface page xv Swgg&sfzoMj ybr zmjfr%cforj owf fmdy xix Acknowledgements xxi 1 Introduction and review
More informationIEOR 6711: Stochastic Models I, Fall 2003, Professor Whitt. Solutions to Final Exam: Thursday, December 18.
IEOR 6711: Stochastic Models I, Fall 23, Professor Whitt Solutions to Final Exam: Thursday, December 18. Below are six questions with several parts. Do as much as you can. Show your work. 1. Two-Pump Gas
More informationA review of Continuous Time MC STA 624, Spring 2015
A review of Continuous Time MC STA 624, Spring 2015 Ruriko Yoshida Dept. of Statistics University of Kentucky polytopes.net STA 624 1 Continuous Time Markov chains Definition A continuous time stochastic
More informationFault-Tolerant Computing
Fault-Tolerant Computing Motivation, Background, and Tools Slide 1 About This Presentation This presentation has been prepared for the graduate course ECE 257A (Fault-Tolerant Computing) by Behrooz Parhami,
More informationContents Preface The Exponential Distribution and the Poisson Process Introduction to Renewal Theory
Contents Preface... v 1 The Exponential Distribution and the Poisson Process... 1 1.1 Introduction... 1 1.2 The Density, the Distribution, the Tail, and the Hazard Functions... 2 1.2.1 The Hazard Function
More informationPerformance Evaluation of Queuing Systems
Performance Evaluation of Queuing Systems Introduction to Queuing Systems System Performance Measures & Little s Law Equilibrium Solution of Birth-Death Processes Analysis of Single-Station Queuing Systems
More informationRandom Walk on a Graph
IOR 67: Stochastic Models I Second Midterm xam, hapters 3 & 4, November 2, 200 SOLUTIONS Justify your answers; show your work.. Random Walk on a raph (25 points) Random Walk on a raph 2 5 F B 3 3 2 Figure
More informationQueueing Theory II. Summary. ! M/M/1 Output process. ! Networks of Queue! Method of Stages. ! General Distributions
Queueing Theory II Summary! M/M/1 Output process! Networks of Queue! Method of Stages " Erlang Distribution " Hyperexponential Distribution! General Distributions " Embedded Markov Chains M/M/1 Output
More informationIMPLICIT DIFFERENTIATION
IMPLICIT DIFFERENTIATION CALCULUS 3 INU0115/515 (MATHS 2) Dr Arian Jannetta MIMA CMath FRAS Implicit Differentiation 1/ 11 Arian Jannetta Explicit an implicit functions Explicit functions An explicit function
More informationModelling Complex Queuing Situations with Markov Processes
Modelling Complex Queuing Situations with Markov Processes Jason Randal Thorne, School of IT, Charles Sturt Uni, NSW 2795, Australia Abstract This article comments upon some new developments in the field
More informationNICTA Short Course. Network Analysis. Vijay Sivaraman. Day 1 Queueing Systems and Markov Chains. Network Analysis, 2008s2 1-1
NICTA Short Course Network Analysis Vijay Sivaraman Day 1 Queueing Systems and Markov Chains Network Analysis, 2008s2 1-1 Outline Why a short course on mathematical analysis? Limited current course offering
More informationQUEUING SYSTEM. Yetunde Folajimi, PhD
QUEUING SYSTEM Yetunde Folajimi, PhD Part 2 Queuing Models Queueing models are constructed so that queue lengths and waiting times can be predicted They help us to understand and quantify the effect of
More informationProblem Set 8
Eli H. Ross eross@mit.edu Alberto De Sole November, 8.5 Problem Set 8 Exercise 36 Let X t and Y t be two independent Poisson processes with rate parameters λ and µ respectively, measuring the number of
More informationThe story of the film so far... Mathematics for Informatics 4a. Continuous-time Markov processes. Counting processes
The story of the film so far... Mathematics for Informatics 4a José Figueroa-O Farrill Lecture 19 28 March 2012 We have been studying stochastic processes; i.e., systems whose time evolution has an element
More informationCOPYRIGHTED MATERIAL CONTENTS. Preface Preface to the First Edition
Preface Preface to the First Edition xi xiii 1 Basic Probability Theory 1 1.1 Introduction 1 1.2 Sample Spaces and Events 3 1.3 The Axioms of Probability 7 1.4 Finite Sample Spaces and Combinatorics 15
More informationBIRTH DEATH PROCESSES AND QUEUEING SYSTEMS
BIRTH DEATH PROCESSES AND QUEUEING SYSTEMS Andrea Bobbio Anno Accademico 999-2000 Queueing Systems 2 Notation for Queueing Systems /λ mean time between arrivals S = /µ ρ = λ/µ N mean service time traffic
More informationMarkovian N-Server Queues (Birth & Death Models)
Markovian -Server Queues (Birth & Death Moels) - Busy Perio Arrivals Poisson (λ) ; Services exp(µ) (E(S) = /µ) Servers statistically ientical, serving FCFS. Offere loa R = λ E(S) = λ/µ Erlangs Q(t) = number
More informationData analysis and stochastic modeling
Data analysis and stochastic modeling Lecture 7 An introduction to queueing theory Guillaume Gravier guillaume.gravier@irisa.fr with a lot of help from Paul Jensen s course http://www.me.utexas.edu/ jensen/ormm/instruction/powerpoint/or_models_09/14_queuing.ppt
More informationSlides 8: Statistical Models in Simulation
Slides 8: Statistical Models in Simulation Purpose and Overview The world the model-builder sees is probabilistic rather than deterministic: Some statistical model might well describe the variations. An
More informationAN M/M/1 QUEUEING SYSTEM WITH INTERRUPTED ARRIVAL STREAM K.C. Madan, Department of Statistics, College of Science, Yarmouk University, Irbid, Jordan
REVISTA INVESTIGACION OPERACIONAL Vol., No., AN M/M/ QUEUEING SYSTEM WITH INTERRUPTED ARRIVAL STREAM K.C. Maan, Department of Statistics, College of Science, Yarmouk University, Irbi, Joran ABSTRACT We
More information