HIV stands for human immunodeficiency virus. The virus attacks the immune system, and weakens our ability to fight infections and disease. HIV/AIDS pro- gresses in body slowly and its symptoms are shown after 6 - 8 years sometimes even later. At present, the most burning issue at the same time, the most dangerous phenomena is Human Immunodeficiency Virus (HIV)  . Since the beginning of the epidemic, more than 70 million people have been infected with the HIV virus and about 35 million people have died of HIV. Globally, 36.7 million [34.0 - 39.8 million] people were living with HIV at the end of 2015  . An estimated 0.8% [0.7% - 0.9%] of adults aged 15 - 49 years worldwide are living with HIV, although the burden of the epidemic continues to vary considerably between countries and regions. Sub-Saharan Africa remains the most severely affected, with nearly 1 in every 25 adults (4.4%) living with HIV and accounting for nearly 70% of the people living with HIV worldwide  . Acquired Immunodeficiency Syndrome (AIDS) was first discovered in 1981, since then it has been considered as the most leading cause of mortality  . A detailed background and survey on HIV/AIDS is described in     . HIV mainly targets CD4+ T cells. The continuous attack HIV causes the depletion of CD4+ T cells and this leads people to gradually become a victim of Acquired Immunodeficiency Syndrome (AIDS). For this reason, the count of CD4+ T cells is considered as the primary indicator of progression of HIV. In recent times, mathematical modeling has become the most powerful tool to incorporate the dynamic behaviors of infectious diseases. Mathematical modeling is basically referred to as a method of simulating real-life situations with mathematical equations to forecast their future behavior  . Numerous mathematical models have been developed to identify the characteristics of human immunodeficiency virus    . HIV dynamic model, a set of ordinary differential equations (ODE) that describe the interaction between HIV virus and human body cells, has been proven useful for understanding the pathogenesis of HIV infection and developing treatment strategies  . In this paper, we have shown the present scenario of HIV/AIDS in Bangladesh. Also we have studied a three-compartmental HIV model and investigated their stability at disease free and endemic equilibrium points.
2. Current Status of HIV Infection in Bangladesh
HIV is a worldwide curse. There is no such country where this pandemic disease does not exist. Although Bangladesh is still considered to be a low responded HIV infected country in world, the present situation indicate that the influence of this pandemic disease is gradually increasing. The main reason for this low prevalence could be the early and sustained HIV prevention programs targeting high risk groups backed by a state-of-the-art surveillance system. Another contributing protective factor could be the high rates of male circumcision. There is, however, a concentrated HIV epidemic among injecting drug users (IDU), primarily due to sharing of unclean syringes and needles. As a result, the rate of new infections is still on the rise and Bangladesh is the only country in the South Asia Region where new infections are rising  .
In Bangladesh, the first case of HIV was detected in 1989  . Since then, it has been enhanced considerably. In 2015 (December 2014 to November 2015), the number of newly HIV infected people is 469 and the number of HIV/AIDS related death is 95. Till December 2015, there were 4143 reported cases of HIV and among them 658 died  . Here we show a graphical representation of HIV surveillance of Bangladesh (see Figure 1) from 1989 to 2015 (except 2008)  .
Figure 1. (a) Number of HIV and AIDS cases from 1989 to 2001; (b) Number of HIV and AIDS cases from 2002 to 2015 (except 2008).
3. Three-Compartmental HIV Model
To generate a realistic model of T cell infection by HIV, we first need to consider the population dynamics of T cells in the absence of HIV. Our interest is to present a mathematical model of HIV infection and analyze the model. In this paper, we present a three compartmental model of HIV which has been taken from  . We have modified this model and added a drug efficacy parameter whose value is in the range between 0 and 1  . The total population size is divided into three stages of HIV/AIDS progression; the susceptible population, HIV infected individuals and HIV virus The total population is given by The population CD4+ T cells starts with a source or production rate and dead cells with rate are reduced from the
susceptible class. It has a logistic growth with where is the
proliferation rate. Parameters and are natural turnover rate of uninfected CD4+ T cells, infected CD4+ T cells and virus. Whereas is the maximum level of CD4+ T cell concentration in the body  . Infected CD4+ T cells it has an infection rate which is concentrated as. The transfer diagram of the model is shown in Figure 2.
Figure 2. Transmission diagram of three compartmental HIV model.
Our modified model is governed by the following ordinary differential equations:
The model is positively invariant and bounded in the region
We have determined the basic reproduction number which was first introduced by Ross (1909), which is defined in epidemiological modeling as the average number of infected individuals produced by one infected immigrant in a population which is completely susceptible  . Finding the basic reproduction number, we can determine the endemic result of disease in populations. If, the disease vanishes and if, the disease spreads and goes to the endemic level.
If one wishes to use a mathematical model to make predictions about a particular individual or population, estimation of model parameters from data is crucial. All the parameters and their values used for model (1) are taken from   and presented in Table 1.
Table 1. Parameters used for model (1).
4. Mathematical Analysis of Model
Here we investigate the positivity of the model, find out different equilibrium points, formulate the basic reproduction number and check the stability at disease free and endemic equilibrium points.
4.1. Positivity of the Solution
Here we check the positivity of each compartments such as susceptible cells, infected and HIV virus. We must have the positive values of these biological compartments. To test the positivity of these biological compartments, we need the following Lemma 1.
Lemma 1. Let then the solutions of the model system of equations (1) are positives.
Proof: To prove the Lemma 1, we have used the system of equations of the model (1).
in order to find the positivity we have,
Multiplying both sides of (2) by we have,
Now Integrating (3)
where is a constant. Applying the initial condition at Hence from (4),
Putting the value of into (4), we get
Hence at and. Similarly we can find the positivity of and under the initial conditions.
Therefore, it is true that,.
4.2. Disease Free Equilibrium Points
The disease free equilibrium of the above HIV model (1) can be obtained by setting
thus we have,
Since we have considered the disease free equilibrium, hence. Thus the above system reduces to,
Thus, the disease free equilibrium is
Again for the endemic equilibrium point, we find, where
Now we calculate the basic reproduction number at.
4.3. Basic Reproduction Number
Basic reproduction number represents the average number of secondary infection caused by a single infected T cell in an entirely susceptible T cell population, throughout its period. In order to find the basic reproduction number of the model (1), we need to identify the classes which are relevant to each other. Form the model (1), we observe that the classes and are relevant. We find the gain and losses of and respectively.
Gains to is, gains to is losses to is and losses to is Now, Matrix for the gain terms:
Since basic reproduction number is to be calculated at disease free equilibrium point, hence
Matrix for the loss terms;
Inverse of is
Now we have to evaluate a matrix such that
Hence the largest eigen value of the matrix is. Thus, the basic the reproduction number of the model (1) is. Now we check the local stability of the model (1) at disease free equilibrium point and chronic infection equilibrium point.
4.4. Local Stability of Disease Free Equilibrium Point
Firstly, we investigate the local stability at disease free equilibrium point but before that we need the following theorem.
Theorem 1: If, the disease free equilibrium point of system (1) is locally asymptotically stable. If, is locally stable and if, then is unstable.
Proof: To prove the above theorem, the following variation matrix is computed corresponding to equilibrium point. From the model (1), let
then the system (1) reduces to,
The Jacobian Matrix of the system (1) is
at, Equation (5) becomes
Now we have to find out the characteristic equation. To do that, first we have to calculate where, is a scalar and is identity matrix. Let, then
To find out the characteristic equation we need to perform, hence
Thus, the characteristic equation is
We observe that, first root of the characteristic equation is
If, then. Also,. Again, hence by Routh-Hurwitz criteria  , locally asymptotically stable. If, then and becomes locally stable. If, then and becomes unstable. Now we investigate the local stability of endemic equilibrium point.
4.5. Local Stability of Chronic Infection Equilibrium Point
Now we investigate the local stability of chronic infection equilibrium point. We need the following Lemma 2.
Lemma 2: Let be a real matrix. If and are all negative, then all of the eigen values of have negative real part  .
Before we apply the Lemma 2, we need the following definition of second additive compound matrix.
Definition 1: Let be an real matrix. The second additive compound matrix of is the matrix defined as follows   :
Theorem 2: The chronic infection equilibrium point of the system (1) is locally asymptotically stable if.
Proof: From Equation (5), we have
at chronic infection equilibrium point,
Now the second additive compound matrix is
Now we compute respectively. Hence
Hence by Lemma 2, is locally asymptotically stable.
5. Numerical Simulations
We have discussed the locally asymptotically stability of both infection free equilibrium and chronic infection equilibrium above. When, the endemic equilibrium may only be stable for small or large. Our numerical solutions consistently show the existence of periodic solutions when is unstable. For the numerical result we use the parametric values used in Table 1 taken from  and  but with the variation of. Considering, we have shown local stability of both the healthy CD4+ T cells and HIV virus at and (see in Figure 3 and Figure 4). Whereas at, is unstable and a periodic solution exists (see in Figure 5).
Figure 3. Using the parameter values of Table 1, is stable, when and.
Figure 4. is stable, when and.
Figure 5. When and a periodic solution is observed.
We observe is unstable within the range of between 0.093453 and 1.9118. From Figure 4, we observe viral load 600 mm−3 persists when while it is below 100 mm−3 at. Again when the initial oscillation disappears after 145+ days whereas at the damped oscillation are clearly visible after 2000 days. We also note that, the values of in these three cases are 0.5081, 0.8227 and 0.48431 respectively.
Bangladesh government and several NGO’s have played a magnificent role in keeping the HIV prevalence low by enhancing awareness to people. But this low prevalence rate is increasing day by day and becoming a great threat to us. In this paper, we have shown a brief report of HIV/AIDS of Bangladesh from 1989 to 2014 (except 2008). Again we have discussed the mathematical presentation of HIV infection in a three-compartmental model. In the model, we added a probability term with the infected T cells. Then we have calculated the basic re-
production number, where is considered as equilibrium of
CD4+ T cells in the absence of HIV infection. At disease free equilibrium point, the model is assumed to be stable and later we conclude the stable and unstable condition for the chronic infected equilibrium points. With the proliferation term and reproduction number, we find the solution of it. We find the numerical solution at different equilibrium points and have observed the curve in periodic and damped oscillation.