Journal of Applied Mathematics
Volume 2018 (2018), Article ID 3420528, 8 pages
https://doi.org/10.1155/2018/3420528

Research Article

A Stochastic TB Model for a Crowded Environment

Sibaliwe Maku Vyambwera and Peter Witbooi

Department of Mathematics and Applied Mathematics, University of the Western Cape, Private Bag X17, Bellville 7535, South Africa

Correspondence should be addressed to Peter Witbooi; pwitbooi@uwc.ac.za

Received 19 February 2018; Accepted 12 May 2018; Published 13 June 2018

Academic Editor: Zhidong Teng

Copyright © 2018 Sibaliwe Maku Vyambwera and Peter Witbooi. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract.

We propose a stochastic compartmental model for the population dynamics of tuberculosis. The model is applicable to crowded environments such as for people in high density camps or in prisons. We start off with a known ordinary differential equation model, and we impose stochastic perturbation. We prove the existence and uniqueness of positive solutions of a stochastic model. We introduce an invariant generalizing the basic reproduction number and prove the stability of the disease-free equilibrium when it is below unity or slightly higher than unity and the perturbation is small. Our main theorem implies that the stochastic perturbation enhances stability of the disease-free equilibrium of the underlying deterministic model. Finally, we perform some simulations to illustrate the analytical findings and the utility of the model.

1. Introduction

Tuberculosis (TB) continues to be a major global health problem that is responsible for 1.5 million deaths worldwide each year [1]. TB is most prevalent in communities with socioeconomical problems but is not confined to such. The authors in [2, 3] associate TB infection with poverty and underdevelopment of some countries. It has been observed globally that one of the major factors driving TB infection is overcrowding. TB mostly occurs in poorest countries that are not developed and particularly where a population is overcrowded and in countries that are influenced by war. Conflict is the most common cause of large population displacement, which often results in relocation to temporary settlements such as camps. Factors including malnutrition and overcrowding in camp settings further increase the exposure to TB infection in these populations. Following up on a paper of Ssematimba et al. [3] regarding internally displaced people’s camps in Uganda, Buonomo and Lacitignola [2] proposed a model that considers the dynamics of TB in concentration camps with a case study in Uganda. Another type of crowded environment which provides favourable conditions for TB to flourish is prisons and more so if the prison is full beyond its capacity. There are more than million inmates in prisons all over the world. The United States of America is in the top rank with about million inmates while South Africa is in rank [4]. South African prison has approximately inmates in custody, of which are sentenced individuals while the rest are awaiting trial. This means that a large number of inmates are kept in remand population and some of them might not be found guilty at the end of the process, after having been exposed to high risk of TB infection.

Mathematical models have been used to model TB by considering the size of the area and how size and density affect the extent to which TB can invade a certain population [2, 3, 5–7]. Quite obviously, considering the manner in which TB is aerially transmitted from one person to another, the prison situation provides favourable conditions for TB to flourish. TB is an infectious disease caused by bacillus Mycobacterium tuberculosis that most often affects the lungs (pulmonary TB) and can affect other parts as well such as brain, kidneys, and spine (extrapulmonary TB) [8, 9]. The TB infection can take place when an infected individual releases some droplet nuclei which can remain airborne in any indoor area for up to four hours. The tubercle bacillus can persist in a dark area for several hours but it is exceptionally sensitive to sunshine. The risk of infection increases as the length of prison stay increases and the sentenced offenders are more likely to get TB infection as compared to the awaiting trial inmates.

Against this background the paper [10] offers a model for the population dynamics of TB in a prison or prison system. In particular, it computes the parameters relevant to South Africa for the given model, using publicly available data. The current paper considers a stochastic form of the model in [10]. It is well understood that stochastic differential equation (sde) attempts to reflect the effect of random disturbances in or on a system. A second reason for studying sde models is that it is good to know that a given model carries some resilience against small disturbances. In this case we consider the transmission parameters to be stochastically perturbed, similarly to [11]. Stochastic pertubation has been studied by Yang and Mao [12]; they considered a multigroup SEIR epidemic model. In most cases, it has been observed in [12, 13] that introducing a stochastic perturbation into an unstable disease-free equilibrium model system of ordinary differential equation may lead to a system being stable in sde. Stochastic differential equation models for various diseases have been studied and similar work has been done in [11, 12, 14–16].

Our paper focuses on the analysis of TB in prisons as prisons have been recognized as institutions with very high TB burden as compared to a general population [17]. For a deterministic model of similar type, in [10] we computed parameter values pertaining to South Africa. For the stochastic model in this paper the focus is on mathematical analysis. In Section 2, the model is introduced, based on the paper of Buonomo and Lacitignola [2]. The existence and uniqueness of the solution to the stochastic models is investigated by using the Lyapunov method in Section 3. Stability of the disease-free equilibrium for stochastic models is shown in Section 4. We show our results by means of numerical simulations and conclude in Section 5.

2. The Model

We introduce a stochastic compartmental model which is based on the deterministic model in the paper of Buonomo and Lacitignola [2]. We divide the population, which is of size at time , into four compartments, namely, the class of susceptible individuals , the class of individuals infected with TB who are not infectious, the class of individuals infected with active TB who are infectious, and the class of individuals under treatment. It is important to note that in general populations removal of individuals out of the system is only by death. In this model, as in [10], the removal is by death or by discharge from prison, and the discharge is the dominant factor. This rate of removal is denoted by . The disease induced mortality rate is denoted by . Individuals are recruited into the susceptible class at a constant rate . Susceptible individuals get infected with active TB at a rate , where is the effective contact rate between the infectious and susceptible individuals. Individuals leave the exposed class for infectious class at rate . Exposed individuals who are infectious move to the infectious class at a rate , where is the effective contact rate between the exposed and infectious individuals. Successfully treated individuals who were infectious move to exposed class at a rate , where is the effective contact rate between the treated and infectious individuals. Exposed and infectious individuals move into class at the rates and , respectively.

Let us assume to be a complete probability space with a filtration which is right continuous. Let be two mutually independent Brownian motions. Let us fix a nonnegative number , which shall serve as the intensity of the perturbation. We also fix two other positive numbers and with that will balance the perturbation. The stochastic perturbations are similar to those in the model of [11].

Model System (1)

It is noticed that if then system (1) does not have a disease-free equilibrium. We will first investigate the model without the inflow of infected cases, i.e., when . In this case the disease-free state

is an equilibrium point. The underlying deterministic model of (1) is the model given by the same system of equations in the special case , i.e., without stochastic perturbation as in [10]. The underlying deterministic model coincides with the model of Buonomo and Lacitignola [2]. The basic reproduction number of the underlying deterministic model has already been computed in paper [2] and is given by the following formula:

where and

We now present the following set:

Remark 1. For the rest of the paper we will assume that the sample paths are restricted to , which is defined as follows:

Lemma 2 (see [13]). For , let be a bounded -valued function and let be any increasing unbounded sequence of positive real numbers. Then there is family of sequences such that for each is a subsequence of and the sequence converges to a chosen limit point of the sequence

3. Existence and Uniqueness of Positive Global Solutions

Proposition 3. Suppose that we have a solution

of system (1) over an interval with and with for all , a.s., then

Proof. Given any solution in satisfying the conditions of Proposition 3, then we have the total population in system (1) obeying the following ordinary differential equation:

Therefore, similarly to [11], for instance, implies that for all

In this section, we investigate the existence and uniqueness of global positive solutions of stochastic models by using the Lyapunov method. This method is popularly applied for such problems; see [23, 24], for instance.

Theorem 4. There is a unique solution to system (1) on for any given initial value , and the solution will remain in with probability one; namely, for all almost surely.

Sketch of the proof. Since the coefficients in (1) satisfy the Lipschitz condition locally, for any given initial value , there is a unique local solution on , where is the explosion time. Our a im is to show that this solution is global and positive almost surely; i.e., a.s.
Let such that , , , For each integer , we define the stopping times

Let

For this purpose we introduce a function as follows:

We note that, by Proposition 3, each of the terms

is positive, and

By Itô’s formula, for all , , we have

After eliminating some negative terms we have the following inequality:

where

and

Taking the integral in (14) from to , we have

By taking expectations, the latter inequality yields

Now we note that

where is the indicator function. If , then there are some components of , , , equal to , and therefore
Thus we have

Combining (14) and (18) gives, for all ,

Letting , we obtain, for all , Hence As a.s. Therefore, the solution of model (1) will not explode at a finite time with probability one. This completes the proof.

4. Stability of Disease-Free Equilibrium

Let us choose a positive number and two nonnegative numbers and . Specific values will be assigned to these numbers in different analyses.

Let us assume that

Now we define a stochastic process

and a process

For , we note that and therefore are defined for all For convenience, we introduce the variables:

and for a stochastic process we shall write

4.1. On the Lyapunov Exponent of

The Lyapunov exponent of a quantity is defined as

The infinitesimal generator of system (1) (see Øksendal [25]) will play an important role in the sequel. Now we can calculate and express it as a function of From Lemma 2 it follows that for each there is an increasing sequence with the following properties (but we shall suppress and write :

For every ,

and the limits below, which shall be denoted by , do exist:

We write

Let

We can write

where

and we note that by the strong law of large numbers [16],

Therefore

Now we expand :

With regard to the calculation of we note the following:

Therefore,

where

This yields the inequality:

In the expression for , if we ignore the multiples of (they are negative), then we obtain an inequality:

4.2. Stability Theorems

We now introduce another invariant , which enables us to formulate stability theorems for the stochastic model (1). As a corollary of the main theorem we can deduce a global stability theorem for disease-free equilibrium. Let

In the model of Buonomo and Lacitignola [2], we have backward bifurcation at . Therefore, the condition does not imply global stability of the underlying deterministic model. As a corollary to the main theorem, Theorem 6, will follow the fact that for the model in [2] the disease-free equilibrium is globally asymptotically stable when . In preparation for our main theorem we introduce a function as follows:

Then

Also we note that

Therefore and we know that . Since has only one critical value on the interval , in view of (44), it follows that the critical point is an absolute minimum of on the interval

Therefore the minimum value of over is

Proposition 5. If

then converges exponentially to zero almost surely.

Proof. We introduce the function of (24), with Now note that (47) is equivalent to

We choose a number sufficiently small such that

Now we choose

From inequality (40) it follows that

where

Now note that we can express as follows:

Therefore, we have

and, consequently,

Therefore

and since and cannot both be zero, it follows that . This completes the proof.

Theorem 6. (a) If almost surely converges exponentially to 0, then

(b) If

then disease-free equilibrium is almost surely exponentially stable.

Proof. (a) Suppose to the contrary that we have

Let be the same as that in (23), with Since almost surely converges exponentially to while

it follows that and (a.s.). Thus from inequality (40) it follows that

Therefore . This implies that converges to , and thus

which is a contradiction. This completes the proof of (a).
(b) This follows from Proposition 5 and Theorem 6(a).

5. Numerical Simulation

The simulations presented here illustrate the analytical results of our model in (1). The parameter values have already been calculated in the paper [10], by using real data, mostly from [18, 20, 21]. We will now use those parameter values, listed in Table 1, and vary the value of and in order for us to be able to find different values of and . We first consider a model without the inflow of infective cases and then with the inflow of infective cases.

Table 1: Model parameters and initial conditions.

Parameter
Estimated value
Source

[10], data from [18, 19]

[10], data from [18, 20]

[10], see also [21]

[10, 22]

Estimated from [10]

[2]

[2]

[2, 21]

[18]

[18]

[10], data from [18]

[10], data from [18]

[10], data from [18]

[10], data from [18]

We give some numerical simulations to show different dynamic outcomes of the deterministic model and its stochastic version. We illustrate by means of simulations the possible disease eradication in the absence of the inflow of infective cases. This will be shown in Figures 1, 2, and 3. Over these three cases we vary the value of and so as to obtain different values of and .

Figure 1: , , , and .

Figure 2: , , and , .

Figure 3: , , and , .

In Figure 1, we present a case in which we take , and then we obtain and This situation does not satisfy the conditions of Theorem 6, and indeed the I-class does not appear to converge to zero. This means that the disease will persist in our prison population.

In Figure 2, we notice that when the perturbation is sufficiently big, then the disease will possibly be eliminated for a stochastic model even if for the deterministic model it does not seem be the case. We have chosen and then we calculate and .

In Figure 3, a choice of and yields and This choice of parameters satisfies the conditions in Theorem 6, and surely the infectious class seems to converge to zero.

We now study model (1) with the inflow of infectives and present a sample computation. We choose as in Table 1 and . Then the values of and can be calculated as . In Figure 4, it is observed that when the basic reproduction number for the underlying deterministic model is above unity, then the disease will persist into our prison system. It is also seen that the inflow of infective cases play a part in influencing the number of TB infected cases in the prison system.

Figure 4: , , and , with , , and .

6. Conclusion

A stochastic SEIT model was presented and analysed to assess the impact of active TB on a crowded environment, specifically in prisons. We started off by verifying that there is a unique global positive solution for the system of stochastic differential equation in (1). It was noted that whenever the basic reproduction number is significantly greater than unity then the disease will persist in the prison population through our simulations in Figures 1 and 2. It has also been observed for a stochastic model that when the perturbation is sufficiently big then the disease tends to vanish and this can be seen in Figure 2. It is more important to study smaller perturbation. It has been observed that whenever , then and almost surely converge exponentially to zero in step with Theorem 6, in the absence of the inflow of infective. These results can also be seen in Figure 3. By introducing the inflow of infective cases into the prison system, TB remains endemic, as can be seen in Figure 4. By screening the inflow on admission and providing for them a separate accommodation, TB infection in a prison system can be greatly reduced.

Data Availability

All the data used in this research are publicly available and are cited in the article. No new data were generated for this article.

Disclosure

This research did not require or request any funding, and no funding was received.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

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