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IEOR 263B, Homework 4 Solution

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<strong>IEOR</strong> <strong>263B</strong>, <strong>Homework</strong> 4 <strong>Solution</strong><br />

Due February 20, 2009<br />

1 Problem 5.3<br />

(i) Imagine that when in state i, dummy (or false) transitions which leave the system in state i occur at rate<br />

M − v i . Then all transitions (real plus dummy) occur at a Poisson rte M and so the number of such<br />

transitions by any time t is finite. Hence, the number of real transitions is also finite with probability 1.<br />

(ii) let X n+1 denotes the time between the n th and n + 1 th transition and let J n denote the state at time n.<br />

If we let<br />

N(t) = sup{n : X 1 + · · · + X n ≤ t}<br />

then N(t) denote the number of transitions by time t. Let j be the first recurrent state that is reached<br />

and suppose it was reached at n 0 transition (which is finite by our assumption). Let n 1 , n 2 , . . . be the<br />

successive integers n at which J n = j. Such integers exist as j is recurrent. Set T 0 = X 1 + · · · + X n0 and<br />

T k = X nk−1 + · · · + X nk . T k is the time between k − 1 th and k th visit to j. It follows that {T k , k ≥ 1}<br />

forms a renewal process and hence ∑ k≥1 T k = ∞ with probability 1. But we have:<br />

∞∑ ∞∑<br />

X n = = ∞<br />

n=1<br />

Hence if the number of transitions are infinite then the time for these transitions is also infinite with<br />

probability one.<br />

2 Problem 5.4<br />

Let T i denote the time to go from i to i + 1, i ≥ 0. Then ∑ N−1<br />

i=0 T i is the time taken to go from 0 to N. As T i<br />

is exponential with rate λ i and the time T i are independent we have:<br />

Also<br />

and<br />

3 Problem 5.5<br />

E<br />

[<br />

exp<br />

(<br />

s<br />

N−1<br />

∑<br />

i=0<br />

T i<br />

)]<br />

k=1<br />

λ i<br />

= Π N−1<br />

i=0 E [exp (sT i)] = Π N−1<br />

i=1<br />

λ i − s<br />

∑<br />

T i =<br />

N−1<br />

E<br />

i=0<br />

N−1<br />

Var<br />

For 0 ≤ s 1 ≤ s 2 . . . ≤ s n ≤ t, we want to calculate<br />

∑<br />

T i =<br />

i=0<br />

N−1<br />

∑<br />

i=0<br />

N−1<br />

∑<br />

P(S i = s 1 , S i+1 = s 2 , . . . , S i+k−1 = s k |X(t) = i + k, X(0) = i)<br />

i=0<br />

1<br />

λ i<br />

1<br />

λ 2 i<br />

which is same as<br />

P(T i = s 1 , T i+1 = s 2 − s 1 , . . . , S i+k−1 = s k − s k−1 , T i+k > t − s k |X(0) = i)<br />

P(X(t) = i + k|X(0) = i)<br />

1


Using the independence of T m ’s and substituting their densities we get:<br />

iλe −iλs1 (i + 1)λe −(i+1)λ(s2−s1) . . . (i + k − 1)λe −(i+k−1)λ(s i+k−s i+k−1 ) e −(i+k)λ(t−s i+k−1)<br />

( )<br />

i + k − 1<br />

e<br />

i − 1<br />

−λti (1 − e −λt ) k<br />

Simplifying we get:<br />

k!Π k λe −λ(t−sn)<br />

m=1<br />

1 − e −λt<br />

4 Problem 5.12<br />

(i) Since P 0 =<br />

state 0),<br />

1/λ<br />

1/λ + 1/mu = µ , it follows from renewal theory (renewal every time we come back to<br />

λ + µ<br />

N(t)<br />

lim = α 0µ<br />

t→∞ t λ + µ + α 1λ<br />

λ + µ<br />

(ii) The expected total time spent in state 0 by time t is<br />

From this:<br />

E[T 0 (t)] =<br />

∫ t<br />

0<br />

P 00 (s)ds = µ<br />

λ + µ t + λ<br />

(<br />

(λ + µ) 2 1 − e (λ+µ)t)<br />

E[N(t)] = α 0 E[T 0 (t)] + α 1 (t − E[T 0 (t)]).<br />

2

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