Applied Mathematics
p-ISSN: 2163-1409 e-ISSN: 2163-1425
2014; 4(3): 86-96
doi:10.5923/j.am.20140403.03
Wiah E. N., Otoo H. Nabubie I. B., Mohammed H. R.
Department of Mathematics, University of Mines and Technology, Tarkwa, Ghana
Correspondence to: Wiah E. N., Department of Mathematics, University of Mines and Technology, Tarkwa, Ghana.
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Copyright © 2014 Scientific & Academic Publishing. All Rights Reserved.
A nonlinear dynamical system and qualitatively analysis of HIV/AIDS epidemic model with treatment is investigated. The model allows for some infected individuals to move from the symptomatic phase to the asymptomatic phase by all sorts of treatment methods. Mathematical analyses establish that the global dynamics of the spread of the HIV infectious disease are completely determined by the basic reproduction number R0. If R0 ≤ 1, the disease free equilibrium is globally stable, where as the unique infected equilibrium is globally asymptotically stable if R0 ≤ 1. Finally, numerical simulations are performed to illustrate the analytical results.
Keywords: Nonlinear Dynamics, HIV\AIDS, Epidemics, Treatment
Cite this paper: Wiah E. N., Otoo H. Nabubie I. B., Mohammed H. R., Nonlinear Dynamics and Chaos in HIV/AIDS Epidemic Model with Treatment, Applied Mathematics, Vol. 4 No. 3, 2014, pp. 86-96. doi: 10.5923/j.am.20140403.03.
, infective
, treated class
and AIDS class
. The detailed transition between these four compartments is depicted in Figure 1. There is an inflow of newly recruited to the susceptible population at a rate
. Moreover, with the introduction of infectives and homogeneous mixing in the population, an individual become infected at rate
. It is assumed that some people are not aware of their HIV status and thus do not seek medical attention. The treated class represents people who seek medical attention. Treatment is the process of offering the HIV positive individual with a life prolonging drug/medicine known as antiretroviral (ARV) medicine or antiretroviral treatment (ART). ART drugs are the main types of treatment for HIV/AIDS. New recruits into the treated class occur at a rate
. Again, people who are ignorant of their HIV status in the infective class are recruited into the AIDS class at rate
. Natural death at the various compartments occurs at a rate
.![]() | Figure 1. Schematics of the Susceptible-Infective-Treated-Aids (SITA) model |
![]() | (1) |
![]() | (2) |
![]() | (3) |
![]() | (4) |
. The total population, N is given by the formula:
From equation (1)-(4) ![]() | (5) |
Hence resulting systems of equations shall be based on![]() | (6) |
![]() | (7) |
![]() | (8) |
then the solutions of
of the system (6)-(8) are positive for all
Proof:Taking the first equation, we have
From the second equation we have
Finally, from the third equation, we have
ProofLet
be any solution of the system with non negative initial conditions then Adding the equations of the system (6)-(8), we have
Hence
Thus the considered region for the system (6)-(8) is
The vector field points to the interior of
on the part of the boundary when
for and is positively invariant.
and the endemic equilibrium by
where
With the natural mortality rate,
considered constant throughout the model, the duration spent in the infectious class is given by 

where
is defined as the spectral radius of the Next Generation Matrix
is the rate of appearance of new infections in compartment
and
is the transfer of individuals out of compartment
by all other means.Given the DFE,
is calculated as the largest eigenvalue (spectral radius) of the matrix of partial derivatives:
where![]() | (9) |
![]() | (10) |
Therefore,
The spectral radius of the next generation matrix is![]() | (11) |
![]() | Figure 2. Phase plane portrait for the classic HIV endemic model with treatment rate σ = 0.01 |
We shall use the linearization approach to proof the local stability of the disease-free equilibrium (DFE). The Jacobian matrix associated with the system (6)-(8) is:
At the DFE, which is given by
we have
Clearly the eigenvalues at the DFE are given by:
For the positive parameters
and
it can be seen that eigenvalues of the DFE are all negative and hence the DFE is stable.Since
we have![]() | (12) |
implies that the inequality (12) also holds and thus we have proved Lemma 4.2.
then the disease-free equilibrium
is globally asymptotically stable in
Proof: Given that
then there exist only the disease free equilibrium
Considering that Lyapunov function candidate
defined as
Differentiating
with respect to time yields
Substituting the system (6)-(8), we have
It is important to note that,
only when
. However, substituting
into the equations for
and
in (6)-(8) shows that
and
as
. Therefore, the maximum invariant set in
is the singleton set
. Hence, the global stability of
when
follows from LaSalle’s invariance principle (Lasalle, 1976 and Tewa et. al. 2009).
Proof. The Jacobian equilibrium is locally asymptotically stable if 
The eigenvalues of
are
Hence, if
then
and
system (6)-(8) is globally asymptotically stable, if
and
and unstable
Proof. Using the constructed Lyapunov function by (Cai, L. and Li, Z., 2010), the global stability of the endemic equilibrium is proved. By defining the Lyapunov function as follows.
By direct calculating the derivative of
along the solution of system (6)-(8) we have;
It implies that ![]() | (13) |
![]() | (14) |

![]() | Figure 3. Population dynamics of the HIV/AIDS epidemic model |
then we obtain
. Noting that
if and only if
therefore the largest compact invariant set
is the singleton
, where
is the endemic equilibrium. Hence by the LaSalle’s invariant principle, it implies that
is globally asymptotically stable in
if
|
. The phase portrait in figure (4a) indicates that the trajectories for any initial populations result in a situation where there are no infective individuals, that is, the disease-free equilibrium. From figure (4b) the phase portrait indicates that for any starting initial value, the solution curves tend to the equilibrium
. Hence, we infer that the system (6)-(8) is globally stable about the endemic equilibrium point
for the set of parameters chosen.![]() | Figure 4a. Phase portrait of the dynamics of susceptibles class and the infective class |
![]() | Figure 4b. Phase portrait of the dynamics of susceptibles class and the treated class |
These values depict the result in figure (5) and show that, increasing treatment rate has the effect of reducing the number of secondary cases and subsequently reduce the HIV/AIDS epidemic. The results further show that increasing the treatment rate decreases the severity of the epidemic as seen by gradual decrease in the peaks and time lags between peaks, as increases.![]() | Figure 5. Disease prevalence in treated class as the rate of treatment increases |
were derived and it was shown that the disease can be eradicated if the basic reproduction is less or equal to unity.(2) The model (6)-(8) has a locally stable disease-free equilibrium whenever the associated reproduction number is less than unity.(3) The DFE of the model (6)-(8) is shown to be globally asymptotically stable when
(4) The endemic equilibrium of the reduced model (6)-(8), is shown to be globally asymptotically stable, when
To explain that treatment may result in the disease persisting or in the disease dying out, depending on parameter value, we simulated the model over different values of the treatment rate
The results shows that increasing the treatment rate decreases the severity of the epidemic as seen by gradual decrease in the peaks and time lags between peaks, as
increases.We conclude that treatment as an intervention strategy can help to contain the HIV/AIDS epidemic but can lead to evolution of drug resistance, which can reverse the benefits of treatment. Although, treatment may lead to evolution of drug resistance, it helps to reduce the proportion of vertically infected and prolongs the lives of all infected individuals.