1. 1 Chapter 5 Continuous time Markov Chains Learning objectives : Introduce continuous time Markov Chain Model manufacturing systems using Markov Chain Able to evaluate the steady-state performances Textbook : C. Cassandras and S. Lafortune, Introduction to Discrete Event Systems, Springer, 2007

2. 2 Plan Basic definitions of continuous time Markov Chains Characteristics of CTMC Performance analysis of CTMC Poisson process Approximation of general distributions by phase type distribution

3. 3 Basic definitions of continuous time Markov Chains

4. 4 Stochastic process Discrete events Continuous event Discrete time Continuous time Memoryless A CTMC is a continuous time and memoriless discrete event stochastic process. Continuous Time Markov Chain (CTMC)

5. 5 Definition : a stochastic process with discrete state space and continuous time {X(t), t > 0} is a continuous time Markov Chain (CTMC) iff P[X(t+s)= j  X(u), 0≤u≤s] = P[X(t+s)= j  X(s)],  t,  s,  j Memoryless: In a CTMC, the past history impacts on the future evolution of the system via the current state of the system

6. 6 Continuous Time Markov Chain (CTMC) Poisson Arrivals Exponential service time N(t) : number of customers at time t Customer Arrivals Customer departures

7. 7 Homogenuous CTMC Definition : A CTMC {X(t), t > 0} is homogeneous iff P[X(t+s)= j  X(t) = i] = P[X(t+s)= j  X(t) = i] = p ij (s) Homogeneous memoryless: In reliability, we only say "a machine that does not fail at age t is as good as new" Only homogeneous CTMC will be considered in this chapter.

8. 8 Characteristics of CTMC

9. 9 Behavior of a CTMC X(t) Two major components: T i = sojourn time in state i (random variable) p ij = probability of moving to state j when leaving state i

10. 10 Sojourn time in a state Let T i be the random variable corresponding to the time spent in state i The memoryless property of the homogenuous CTMC implies The exponential distribution is the only continuous probability distribution having this property. In an CTMC, the sojourn time in any state is exponentially distributed.

11. 11 Exponential distribution Let T be a continuous random variable with an exponential distribution of parameter Distribution Function (figure) : F T (t) = P{T ≤ t} Probability density function : f T (t) = dF T (t)/dt Mean : E[T] = 1/  Standard deviation:  [T] = 1/  Coeficient of variation: Cv(T) =  [T]/ E[T] = 1 Parameter often corresponds to some event rate (failure rate, repair rate, production rate,...)

12. 12 Exponential distribution Memoryless : For a machine with exponentially distributed lifetime, we say that it is "as good as new" if it is not failed. The remaining lifetime of an used but UP machine has the same distribution as a new machine.

13. 13 Transition probability Whe a CTMC leaves state i, it jumps to state j with probability p ij. This probability is: independent of time as the CTMC is homogeneous independent of sojourn time Ti as the process is markovian (memoryless)

14. 14 1st characterization of a CTMC An CTMC is fully characterized by the following parameters: {  i } i  E with  i as the parameter of the exponential distribution of sojourn time T i {p ij } i≠j, with pij as the transition probability from i to j when leaving state i

15. 15 Classification of a CTMC Each CTMC is associated an underlying DTMC by neglecting sojourn times. A state i of a CTMC is said transient (resp. recurrent, absorbing) if it is transient (resp. recurrent, absorbing) in the underlying DTCM A CTMC is irreducible if its underlying DTMC is irreducible. Remark: the concept of periodicity is not relevant.

16. 16 2nd characterization of a CTMC Each state activates several potential events leading to different transitions. A CTMC travels from state i to state j in T ij time, an exponentially distributed random variable with parameter  ij.  i is called transition rate from i to j.

17. 17 Equivalence of the two representation Let T i = MIN j {T ij } p ij = P{T ij = T i } Result to prove: T i = EXP(  ij ), p ij is independent of T i Moment generating function M X (u) = E[exp(uX)]

18. 18 Performance analysis of CTMC

19. 19 Probability distribution State probability  i (t) = P{X(t) = i} state probability vector, also called probability distribution  (t) = (  1 (t),  2 (t),...)

20. 20 Transient analysis By conditionning on X(t), With

21. 21 Transient analysis It can be shown, Letting dt go to 0,

22. 22 Infinitesimal generator Let The matrix Q = [q ij ] is called infinitesimal generator of the CTMC As a ressult,

23. 23 Steady state distribution of a CTMC Thereom: For an irreducible CTMC with postive recurrent states, the probability distribution converges to a vector of stationary probabilities (  1,  2,...) that is independent of the initial distribution  (0). Further it is the unique solution of the following equation system: normalization equation flow balance equation or equilibrium eq

24. 24 Flow balance equation The balance equation equivalent to :  i≠j  j  ji =  i≠j  i  ij Associate to each transition (i,j) a probability flow :  i  ij  i≠j  j  ji : total flow into state i  i≠j  i  ij : total flow out of state i Interpretation : Total flow in = Total flow out

25. 25 Flow balance equation of set of states Let E 1 be a subset of states Flow balance equation : Total flow into E 1 = Total flow out of E 1

26. 26 A manufaturing system Consider a machine which can be either UP or DOWN. The state of the machine is checked continuously. The average time to failure of an UP machine is 10 days. The average time for repair of a DOWN machine is 1.5 days. Determine the conditions for the state of the machine {X(t)} to be a Markov chain. Draw the Markov chain model. Find the transient distribution by starting from state UP and DOWN. Check whether the Markov chain is recurrent. Determine the steady state distribution. Determine the availability of the machine.

27. 27 Poisson process

28. 28 Poisson process A Poisson process is a stochastic process N(t) such that N(0) = 1 N(t) increments by +1 after a time T random distributed according to an exponential distribution of parameter. An arrival process is said Poisson if the inter-arrival times are exponentially distributed.

29. 29 Properties of Poisson process A Poisson process is an irreducible CTMC N(t) has a Poisson distribution with parameter t

30. 30 Properties of Poisson process A Poisson process is an irreducible CTMC P{N(t+dt) = k+1 | N(t) = k} = dt + o(dt) Probability of 0 arrival in dt P{N(t+dt) = k | N(t) = k} = 1- dt + o(dt) Probability of more than one arrival in dt P{N(t+dt) > k+1 | N(t) = k} = o(dt)

31. 31 Properties of Poisson process The superposition of n Poisson process of parameter i is a Poisson process of parameter  i Assume that a Poisson process is split into n processes with probabilities p i. These n process are independent Poisson process with parameter p i

32. 32 Birth-Death process

33. 33 Definition Consider a population of individuals Let N(t) be the size of the population with N(t) = 0, 1, 2,... When N(t) = n, births arrive at according to a Poisson pocess of birth rate n > 0 Deaths arrive also according to a Poisson process of death rate  n > 0.

34. 34 Key issues Graphic representation of the Markov chain Relation with the Poisson process (also called pure birth process) Condition for existence of steady state distribution Sufficient condition (larger death rate than birth rate) Steady state distribution  n

35. 35 Approximation of general distributions by phase type distribution

36. 36 Phase-type distribution A probaiblity distribution that results from a system of one or more inter-related Poisson process occurring in sequence, or phases. The sequence in which each of the phases occur may itself be a stochastic process. Phase distribution = time until the absorption of a CTMC one absorbing state. Each of the states of the Markov process represents one of the phases. Phase-type distributions can be used to approximate any positive valued distribution.

37. 37 Definition A CTMC with m+1 states, where m ≥ 1, such that the states 1,...,m are transient states and state m+1 is an absorbing state. An initial probability of starting in any of the m+1 phases given by the probability vector (α, α m+1 ). The continuous phase-type distribution is the distribution of time from the above process's starting until absorption in the absorbing state. This process can be written in the form of a transition rate matrix, where S is an m×m matrix and S 0 = -S 1 with 1 represents an m×1 vector with every element being 1

38. 38 Characterization Time X until the absorbing state is phase-type distributed PH(α,S). The distribution function of X is given by, F(x) = 1 -  exp(Sx)1, and the density function, f(x) =  exp(Sx)S 0, for all x > 0.

39. 39 Erlang distribution E k : k-stage Erlang distribution with parameter  X = sum of k independent random variable of exponential distribution with parameter  E[X] = k/  Var[X] = k/  2 C X =  X / E[X] = 1/k 1/2  ●●●

40. 40 Hyper-exponential or mixture of exponential distribution X =  1 X 1 +  2 X 2... +  n X n where  1 +  2... +  n = 1, X i = EXP(  i ) E[X] =  1 /  1 +  2 /  2... +  n /  n Var[X] =  1 /  1 2 +  2 /  2 2... +  n /  n 2

41. 41 Coxian distribution nn ●●● p1p2p n-1 1-p 1 1-p 2 1 Coxian distribution can be used to approximate any distribution.

42. 42 A manufaturing system Consider a machine which can be either UP or DOWN. The state of the machine is checked continuously. The average time to failure of an UP machine is 10 days. The average time for repair of a DOWN machine is 1.5 days. Assumed that UP time = E 2 and DOWN time = E 3. Draw the Markov chain model.