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Consider a birth and death process with birth rates \(\lambda_{i}=(i+1) \lambda, i \geqslant 0\), and death rates \(\mu_{i}=i \mu, i \geqslant 0\) (a) Determine the expected time to go from state 0 to state 4 . (b) Determine the expected time to go from state 2 to state 5 . (c) Determine the variances in parts (a) and (b).

Short Answer

Expert verified
The expected time to go from state 0 to state 4 is \(t_{0 \rightarrow 4} = \frac{1 + \frac{\mu_1}{\lambda_1} + \frac{\mu_2}{\lambda_2} + \frac{\mu_3}{\lambda_3}}{\lambda_0 + \mu_0 + \lambda_1 + \mu_1 + \lambda_2 + \mu_2 + \lambda_3 + \mu_3}\), while the expected time to go from state 2 to state 5 is \(t_{2 \rightarrow 5} = \frac{1 + \frac{\mu_3}{\lambda_3} + \frac{\mu_4}{\lambda_4} + \frac{\mu_5}{\lambda_5}}{\lambda_2 + \mu_2 + \lambda_3 + \mu_3 + \lambda_4 + \mu_4 + \lambda_5 + \mu_5}\). The variances are given by \(Var_{0 \rightarrow 4} = \sum_{i=0}^{3}P_{i, i+1}(1 + t_{0 \rightarrow 4} - t_{i \rightarrow 4})^2\) and \(Var_{2 \rightarrow 5} = \sum_{i=2}^{4}P_{i, i+1}(1 + t_{2 \rightarrow 5} - t_{i \rightarrow 5})^2\).

Step by step solution

01

Understand the birth and death process

A birth and death process is a special case of continuous-time Markov chain that models instantaneous events of "birth" and "death." In this case, "birth" is represented by moving from one state to a larger one, and "death" is going back to a smaller state. We are given the birth rates \(\lambda_i = (i+1)\lambda\) and death rates \(\mu_i = i\mu\).
02

Calculate the transition probabilities

To find the transition probabilities, we need to use the birth rates and death rates. The probability of moving from state i to state i+1 is given by: \(P_{i, i+1} = \frac{\lambda_i}{\lambda_i + \mu_i} = \frac{(i+1)\lambda}{(i+1)\lambda + i\mu}\) And similarly, the probability of moving from state i to state i-1 is given by: \(P_{i, i-1} = \frac{\mu_i}{\lambda_i + \mu_i} = \frac{i\mu}{(i+1)\lambda + i\mu}\)
03

Calculate the expected time to go from state 0 to state 4

To find the expected time to go from state 0 to state 4, we need to calculate the expected number of steps and divide it by the sum of the birth rates and death rates. The expected number of steps is given by: \(E_{0 \rightarrow 4} = E_{0,1} + E_{1,2} + E_{2,3} + E_{3,4}\) Each of these expectations can be calculated using: \(E_{i, i+1} = 1 + \frac{\mu_i}{\lambda_i}E_{i-1,i}\) We can then plug in the values for birth rates and death rates: \(E_{0 \rightarrow 4} = 1 + \frac{\mu_0}{\lambda_0}E_{-1,0} + \frac{\mu_1}{\lambda_1}E_{0,1} + \frac{\mu_2}{\lambda_2}E_{1,2} + \frac{\mu_3}{\lambda_3}E_{2,3}\) We know that \(E_{-1,0} = 0\), so we can simplify: \(E_{0 \rightarrow 4} = 1 + \frac{\mu_1}{\lambda_1} + \frac{\mu_2}{\lambda_2} + \frac{\mu_3}{\lambda_3}\) Finally, we can compute the expected time by dividing by the sum of the birth rates and death rates: \(t_{0 \rightarrow 4} = \frac{E_{0 \rightarrow 4}}{\lambda_0 + \mu_0 + \lambda_1 + \mu_1 + \lambda_2 + \mu_2 + \lambda_3 + \mu_3}\)
04

Calculate the expected time to go from state 2 to state 5

Similarly, we can calculate the expected time to go from state 2 to state 5 as: \(t_{2 \rightarrow 5} = \frac{1 + \frac{\mu_3}{\lambda_3} + \frac{\mu_4}{\lambda_4} + \frac{\mu_5}{\lambda_5}}{\lambda_2 + \mu_2 + \lambda_3 + \mu_3 + \lambda_4 + \mu_4 + \lambda_5 + \mu_5}\)
05

Calculate the variances in parts (a) and (b)

We can calculate the variances using the transition probabilities and the expected times: \(Var_{0 \rightarrow 4} = \sum_{i=0}^{3}P_{i, i+1}(1 + t_{0 \rightarrow 4} - t_{i \rightarrow 4})^2\) \(Var_{2 \rightarrow 5} = \sum_{i=2}^{4}P_{i, i+1}(1 + t_{2 \rightarrow 5} - t_{i \rightarrow 5})^2\)
06

Conclusion

In this exercise, we have determined the expected time to go from state 0 to state 4 and from state 2 to state 5, as well as the variances for these transitions in a given birth and death process. The most important steps involved calculating the transition probabilities and then using these probabilities to determine the main quantities of interest.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Continuous-Time Markov Chain
Imagine a system where events occur randomly over time; such a system can be modeled by a mathematical construct known as a continuous-time Markov chain (CTMC). The essence of a CTMC lies in the memoryless property, signifying that the system's future behavior only depends on its present state and not on how it got there.

Moreover, in a CTMC, changes between states occur continuously over time, and each state transition is driven by a probability mechanism. These transitions are analogous to the ticking of a clock with a random interval between each tick. In the context of a birth and death process, such transitions represent natural phenomena like population growth or queue dynamics, where 'birth' increases the population or queue length and 'death' decreases it. Applying this concept to real-life examples, you can think of CTMC as a fluctuating population of animals in an ecosystem or customers in line at a store, with arrivals and departures happening at unpredictable moments.
Transition Probabilities
Transition probabilities are the core of understanding Markov chains. These probabilities dictate the likelihood of the system moving from one state to another. Specifically, for a birth and death process, the transition probabilities between states determine how likely it is for the system to experience a 'birth' (move to a higher state) or a 'death' (move to a lower state).

These probabilities are not static and often depend on the current state of the system. For instance, in our exercise, the transition probability from state i to state i+1 and i to state i-1 are calculated using the birth and death rates, respectively. This nuanced relationship between the states and their transition probabilities highlights the importance of the respective rates as they fundamentally influence the structure and the behavior of the Markov chain.
Expected Time to Absorption
One of the intriguing aspects of Markov chains, especially in birth and death processes, is the notion of 'absorption', which occurs when the system enters a state from which it cannot leave. However, in many practical cases, we deal with 'transient' states, where the system eventually moves to another state. The expected time to absorption, or transition between states, is a measure of how long it will take, on average, before a certain event occurs.

In the exercise we're considering, we're not looking at absorption but at the expected time to transition from state 0 to state 4 and state 2 to state 5. The calculations involved are focused on finding the mean time required for these state changes, which are crucial for predicting system behavior over time and planning according to those predictions. Knowing these expected times helps in understanding the dynamics of processes such as queue waiting times or population growth.
Variance of Transition Times
The variance of transition times is just as critical as the expected times when examining a birth and death process. While the expected time gives us an average, the variance provides us with a measure of how spread out the transition times can be. A high variance indicates that the actual transition time can deviate significantly from the average, leading to uncertainty in the system's behavior.

By calculating the variance, as done in the exercise, we gain insights into the reliability and predictability of the process. If you're managing a service system, for instance, knowing the variance in customer service times can help in resource allocation like opening new service counters to minimize wait times. In ecological terms, knowing the variance helps in predicting population fluctuations, which can be crucial for conservation efforts. Understanding both the expected time and its variance allows for better preparation and response to the diverse outcomes within a birth and death process.

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Most popular questions from this chapter

Potential customers arrive at a full-service, one-pump gas station at a Poisson rate of 20 cars per hour. However, customers will only enter the station for gas if there are no more than two cars (including the one currently being attended to) at the pump. Suppose the amount of time required to service a car is exponentially distributed with a mean of five minutes. (a) What fraction of the attendant's time will be spent servicing cars? (b) What fraction of potential customers are lost?

Consider a set of \(n\) machines and a single repair facility to service these machines. Suppose that when machine \(i, i=1, \ldots, n\), fails it requires an exponentially distributed amount of work with rate \(\mu_{i}\) to repair it. The repair facility divides its efforts equally among all failed machines in the sense that whenever there are \(k\) failed machines each one receives work at a rate of \(1 / k\) per unit time. If there are a total of \(r\) working machines, including machine \(i\), then \(i\) fails at an instantaneous rate \(\lambda_{i} / r\) (a) Define an appropriate state space so as to be able to analyze the preceding system as a continuous-time Markov chain. (b) Give the instantaneous transition rates (that is, give the \(\left.q_{i j}\right)\). (c) Write the time reversibility equations. (d) Find the limiting probabilities and show that the process is time reversible.

Let \(Y\) denote an exponential random variable with rate \(\lambda\) that is independent of the continuous-time Markov chain \(\\{X(t)\\}\) and let $$ \bar{P}_{i j}=P[X(Y)=j \mid X(0)=i\\} $$ (a) Show that $$ \bar{P}_{i j}=\frac{1}{v_{i}+\lambda} \sum_{k} q_{i k} \bar{P}_{k j}+\frac{\lambda}{v_{i}+\lambda} \delta_{i j} $$ where \(\delta_{i j}\) is 1 when \(i=j\) and 0 when \(i \neq j\) (b) Show that the solution of the preceding set of equations is given by $$ \overline{\mathbf{P}}=(\mathbf{I}-\mathbf{R} / \lambda)^{-1} $$ where \(\overline{\mathbf{P}}\) is the matrix of elements \(\bar{P}_{i j}, \mathbf{I}\) is the identity matrix, and \(\mathbf{R}\) the matrix specified in Section \(6.8\). (c) Suppose now that \(Y_{1}, \ldots, Y_{n}\) are independent exponentials with rate \(\lambda\) that are independent of \(\\{X(t)\\}\). Show that $$ P\left[X\left(Y_{1}+\cdots+Y_{n}\right)=j \mid X(0)=i\right\\} $$ is equal to the element in row \(i\), column \(j\) of the matrix \(\overline{\mathbf{p}}^{n}\). (d) Explain the relationship of the preceding to Approximation 2 of Section \(6.8\).

In Example \(6.20\), we computed \(m(t)=E[O(t)]\), the expected occupation time in state 0 by time \(t\) for the two-state continuous-time Markov chain starting in state 0\. Another way of obtaining this quantity is by deriving a differential equation for it. (a) Show that $$ m(t+h)=m(t)+P_{00}(t) h+o(h) $$ (b) Show that $$ m^{\prime}(t)=\frac{\mu}{\lambda+\mu}+\frac{\lambda}{\lambda+\mu} e^{-(\lambda+\mu) t} $$ (c) Solve for \(m(t)\).

Suppose that a one-celled organism can be in one of two states-either \(A\) or \(B\). An individual in state \(A\) will change to state \(B\) at an exponential rate \(\alpha ;\) an individual in state \(B\) divides into two new individuals of type \(A\) at an exponential rate \(\beta .\) Define an appropriate continuous- time Markov chain for a population of such organisms and determine the appropriate parameters for this model.

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