Applied Mathematical Sciences, Vol. 9, 2015, no.
81, 3997 - 4008
                HIKARI Ltd, www.m-hikari.com
           http://dx.doi.org/10.12988/ams.2015.54334
  Global Analysis of a HCV Model with CTL,
            Antibody Responses and Therapy
                                     Adil Meskaf
Department of Mathematics, Faculty of Sciences and Techniques, Mohammedia
   University Hassan II-Casablanca, P.O. Box 146, Mohammedia, Morocco
                                   Youssef Tabit
           Department of SEG, Faculty Polydisciplinary of El Jadida
              University Chouaib Doukkali, El jadida, Morocco
                                    Karam Allali
Department of Mathematics, Faculty of Sciences and Techniques, Mohammedia
   University Hassan II-Casablanca, P.O. Box 146, Mohammedia, Morocco
    Copyright c 2015 Adil Meskaf et al. This article is distributed under the Creative Com-
mons Attribution License, which permits unrestricted use, distribution, and reproduction in
any medium, provided the original work is properly cited.
                                       Abstract
          In this paper, the global analysis of a HCV model with CTLs, anti-
      body responses and therapy is studied. We incorporate into our model
      two treatments; the aim of the first one is to reduce the infected cells,
      while the second is to block the virus. We prove that the solutions with
      positive initial conditions are all positive and bounded. Moreover, we
      establish by using some appropriate Lyapunov functions that with the
      therapy the model becomes more stable than the one without treatment.
    Mathematics Subject Classification: 34D23, 34K20, 92B05, 92D30
   Keywords: Basic infection reproduction number, CTL and antibody re-
sponses, HCV model, stability, therapy
3998                                                            Adil Meskaf et al.
1      Introduction
Hepatitis C is a liver disease caused by the hepatitis C virus (HCV). Approx-
imately, 130 − 150 million people globally have chronic hepatitis C infection.
Therefore, HCV infection presents a significant global public health issue [6].
For this reason, many mathematical models have been developed in order to
understand the HCV dynamics [1, 5, 9]. In this article, we will consider the
basic model presented by Wodarz in [9] and we will continue the investigation
by introducing therapy into the model. It is well known that the antiviral
therapies combined with interferon and ribavirin are successful in 90% of per-
sons with acute infection and in 50% cases of persons with chronic infection
[2]. The model of the HCV dynamics that we consider is under the following
form:
                       dX
                     
                     
                             = λ − dX − β(1 − u1 )V X,
                     
                     
                       dt
                       dY
                     
                     
                              = β(1 − u1 )V X − aY − pY Z,
                     
                     
                     
                     
                     
                       dt
                        dV
                     
                              = k(1 − u2 )Y − δV − qV W,                      (1)
                     
                       dt
                       dW
                     
                     
                              = gV W − hW,
                     
                     
                     
                     
                     
                       dt
                      dZ
                     
                     
                              = cY Z − bZ,
                     
                         dt
    the problem is supplemented by the initial conditions:
          X(0) = X0 , Y (0) = Y0 , V (0) = V0 , Z(0) = Z0 , W (0) = W0 .
    This model contains five variables, that is, uninfected cells (X), infected
cells (Y), free virus (V), an antibody response (W) and a CTL response (Z).
Susceptible host cells (X) are produced at a rate λ, die at a rate dX and become
infected by virus at a rate βXV . Infected cells die at a rate aY and are killed
by the CTL response at a rate pY Z. Free virus is produced by infected cells
at a rate kY and decays at a rate δV and is neutralized by antibodies at a rate
qV W . CTLs expand in response to viral antigen derived from infected cells
at a rate cY Z and decay in the absence of antigenic stimulation at a rate bZ.
Antibodies develop in response to free virus at a rate gV W and decay at a rate
hW . The parameter u1 represents the efficiency of drug therapy in blocking
new infection, so that infection rate in the presence of drug is β(1 − u1 ), while
the parameter u2 stands for the efficiency of drug therapy in inhibiting viral
production, such that the virion production rate under therapy is k(1 − u2 ).
    Clearly, the system (1) has a basic infection reproductive number of
Global analysis of a HCV model with CTL, antibody responses and therapy 3999
                                 λβk(1 − u1 )(1 − u2 )
                                    R0 =               .
                                          daδ
    The present paper is organized as follows. In section 2, we study the global
existence of solutions, followed in section 3 by the analysis of the model. We
discuss and conclude in the last section.
2      The global existence of solutions
In order to prove the global existence of solutions, we study the positivity
and boundedness of solutions of system (1) describing the evolution of the cell
population. For biological reasons, we assume that the initial data for this
model satisfy :
                     X0 ≥ 0, Y0 ≥ 0, V0 ≥ 0, W0 ≥ 0, Z0 ≥ 0.
Proposition 1. All solutions with non-negative initial conditions exist for all
t > 0 and remain bounded and non-negative. Moreover we have
    i) X(t) ≤ X0 + λd ,
    ii) Y (t) ≤ Y0 + max(1, 2 − ad )X0 + max( λa , λd ),
                      k(1−u2 )
 iii) V (t) ≤ V0 +       δ
                                    kY k∞ ,                                                                                        
 iv) W (t) ≤ W0 +         g
                          q
                                  max(1; 2 −    δ
                                                h
                                                  )V0   +   max( k(1−u
                                                                    δ
                                                                      2 ) k(1−u2 )
                                                                         , h ) kY    k∞ ,                                                                                                  
                      c                       d
    v) Z(t) ≤ Z0 +    p
                              max(1; 2 −      b
                                                )X0 + Y0 + max( λb , λd ) + max(0; 1 − ab ) kY   k∞ .
   Proof
For positivity, we show that any solution starting in non negative orthant
R5+ = {(X, Y, V, W, Z) ∈ R5 : X ≥ 0, Y ≥ 0, V ≥ 0, W ≥ 0, Z ≥ 0} remains
there forever. In fact, (X(t), Y (t), V (t), W (t), Z(t)) ∈ R5+ we have
Ẋ |X=0 = λ ≥ 0, Ẏ |Y =0 = β(1 − u1 )V X ≥ 0, V̇ |V =0 = k(1 − u2 )Y ≥ 0,
Ẇ |W =0 = 0 ≥ 0, Ż |Z=0 = 0 ≥ 0
Hence, positivity of all solutions initiating in R5+ is guaranteed [?].
   From the first equation of the system (1), we deduce that Ẋ + dX ≤ λ,
then dtd (Xedt ) ≤ λedt .
Hence,
                                                    λ
                                  X(t) ≤ X0 e(−dt) + (1 − e−dt ),
                                                    d
4000                                                                                        Adil Meskaf et al.
Since 0 ≤ e−dt ≤ 1, we deduce (i).
From the first and second equation of the system (1), we have
                                  Ẏ + aY ≤ λ − dX − Ẋ.
Thus,
                                                         Rt
                  Y (t)eat − Y0 ≤ λa (eat − 1) −          0
                                                                      d
                                                              e(a−d)s ds (X(s)eds )ds.
Using the integration by parts, we get
         Rt              d
                                                                                Rt
             0
                 e(a−d)s ds (X(s)eds )ds = [X(s)eas ]t0 − (a − d)                 0
                                                                                      X(s)eas ds.
Therefore,
                                                                                 Z    t
                          −at    λ
  Y (t) ≤ (X0 + Y0 )e           + (1 − e−at ) − X(t) + (a − d)                            X(s)ea(s−t) ds. (2)
                                 a                                                0
   If a − d ≤ 0, then
                                                       λ
                                      Y (t) ≤ X0 + Y0 + .                                                 (3)
                                                       a
   If a − d ≥ 0, then
                                              λ
                                                                  Rt
                     Y (t) ≤ X0 + Y0 +        a
                                                  + (a − d)        0
                                                                        X(s)ea(s−t) ds.
According to i), we have
                                                      (a−d)
                     Y (t) ≤ X0 + Y0 +        λ
                                              a
                                                  +     a
                                                            (X0        + λd )(1 − e−at ),
hence,
                                                 d     λ
                                Y (t) ≤ Y0 + (2 − )X0 + .                                                 (4)
                                                 a     a
From (3) and (4), we deduce (ii).
Now, we prove iii). The third equation of system 1, and (V (t), Z(t)) ∈ R2+ ,
imply that
                                                              Z    t
                                      −δt
                       V (t) ≤ V0 e         + k(1 − u2 )               Y (s)e(s−t) ds,
                                                               0
then
                                             k(1−u2 )
                          V (t) ≤ V0 +          δ
                                                        kY k∞ (1 − e−tδ ).
Global analysis of a HCV model with CTL, antibody responses and therapy 4001
Since 1 − e−tδ ≤ 1, we deduce (iii).
Using a same technique to show (2), we get
                   g t 
                      Z
             −ht
                           k(1 − u2 )Y (s) + (h − δ)V (s) eh(s−t) ds − V (t) + V0 e−ht .
                                                         
W (t) = W0 e +
                   q 0
                                                                               (5)
   If h − δ ≤ 0, then
                                                          
                                 g k(1 − u2 )
                   W (t) ≤ W0 +                 kY k∞ + V0 .                   (6)
                                 q        h
If h − δ ≥ 0, using (iii), we have
                                                                                            g k(1 − u2 )             δ
                W (t) ≤ W0 +                 kY k∞ + (2 − )V0 .                (7)
                                q     δ                  h
   From (6) and (7), we deduce (iv).
Finally, we prove v). The the fifth equation of system (1) implies that                                                            
                                  c
               Ż + bZ = cY Z = p λ − (Ẋ + dX) − (Ẏ + aY ) .
Using the same techniques for the proof of (2) and (5), we get
                                     Z t                                         
          c         λ        −bt c λ                            b(s−t)
Z(t) = (X0 +Y0 − )+Z0 e +             + [(b−d)X(s)+(b−a)Y (s)]e        ds−X(t)−Y (t) .
          p         b             p b 0
                                                                        (8)
If b − d ≤ 0 and b − a ≤ 0, we have
                                                  
                                    c λ
                       Z(t) ≤ Z0 +       + X 0 + Y0 .
                                    p b
If b − d ≤ 0 and b − a ≥ 0, we have
                                                        
                             c λ                 a
               Z(t) ≤ Z0 +       + X0 + Y0 + (1 − ) kY k∞ .
                             p b                 b
   If b − d ≥ 0 and b − a ≤ 0, we have
                                                   
                                 c λ       d
                    Z(t) ≤ Z0 +      + (2 − )X0 + Y0 .
                                 p d       b
If b − d ≥ 0 and b − a ≥ 0, we have
                                                          
                         c λ        d              a
            Z(t) ≤ Z0 +      + (2 − )X0 + Y0 + (1 − ) kY k∞ .                  (9)
                        p d         b              b
From (8) and (9), we deduce (v).
4002                                                              Adil Meskaf et al.
3      Analysis of the model
In this section, we will prove that there exist a disease free equilibrium point
and four endemic equilibrium points. Next, we will study the global stability
of these equilibrium points.
   By a simple calculation, the system (1) has always one disease-free equilib-
rium
E0 = ( λd , 0, 0, 0, 0) and four endemic equilibrium points:
    E1 = (X1 , Y1 , V1 , 0, 0) where
               aδ                   λkβ(1 − u1 )(1 − u2 ) − adδ        λkβ(1 − u1 )(1 − u2 ) − adδ
X1 =                         , Y1 =                             , V1 =                             .
        kβ(1 − u1 )(1 − u2 )          akβ(1 − u1 )(1 − u2 )                  βδa(1 − u1 )
E2 = (X2 , Y2 , V2 , 0, Z2 ) where
                             λδc                   b       k(1 − u2 )b
             X2 =                            , Y2 = , V2 =              ,
                 dδc + kβb(1 − u1 )(1 − u2 )       c            δc
                kβλc(1 − u1 )(1 − u2 ) − a(dδc + βkb(1 − u1 )(1 − u2 ))
           Z2 =                                                         .
                            p[dδc + βkb(1 − u1 )(1 − u2 )]
    E3 = (X3 , Y3 , V3 , 0, Z3 ) where
                               λg                    λβ(1 − u1 )h
                        X3 =              , Y3 =
                         dg + βh(1 − u1 )         a(dg + β(1 − u1 )h)
               h       gkλβ(1 − u1 )(1 − u2 ) − δa(dg + β(1 − u1 )h)
           V3 = , W3 =                                               .
               g                  aq(dg + β(1 − u1 )h)
E4 = (X4 , Y4 , V4 , W4 , Z4 ) where
                                                λg               b       h
                                         X4 =              , Y4 = , V4 =
                                          dg + β(1 − u1 )h       c       g
            kbg(1 − u2 ) − δhc        cβhλ(1 − u1 ) − ab(dg + β(1 − u1 )h)
       W4 =                    , Z4 =                                      .
                   cqh                       (dg + β(1 − u1 )h)pb
    In order to study the global stability of the points E1 , E2 , E3 and E4 , we
define the following numbers:
                                      λk(1 − u2 )g
                               
                                  W
                                D0 =              ,
                               
                               
                                          aδh
                                            1                                   (10)
                                  W
                                H0 =              ,
                               
                                         1
                                            + D1W
                               
                                         R0         0
Global analysis of a HCV model with CTL, antibody responses and therapy 4003
                                                                     λc
                                     
                                        Z
                                      D0 =                             ,
                                     
                                     
                                                                     ab
                                                               1                                             (11)
                                        Z
                                      H0 =                                ,
                                     
                                                         1         1
                                                          R0
                                                               +   D0Z
   Then, these equilibria can be written as follows:
                  Ei = ( λd QX   λ Y d V δ W a Z
                             i , a Qi , β Qi , q Qi , p Qi ), 0 ≤ i ≤ 4,
   where
                         QX       Y    V    W    Z
                          0 = 1, Q0 = Q0 = Q0 = Q0 = 0,
                      1                        1
            QX
             1 =      R0
                         , QY1   =1−           R0
                                                  , QV1   = R0 − 1, QW    Z
                                                                     1 = Q1 = 0,
                     H0Z              1                R0
           QX
            2 =      R0
                         , QY2   =   D0Z
                                         , QV2     =   D0Z
                                                           , QW
                                                              2        = 0, QZ2 = H0Z − 1,
                   H0W               H0W               R0
           QX
            3 =    R0
                         , QY3 =     D0W
                                           , QV3 =     D0W
                                                               , QW    W       Z
                                                                  3 = H0 − 1, Q3 = 0,
            H0W              1                  R0                   D0W                    D0Z
     QX
      4 =   R0
                  , QY4 =   D0Z
                                , QV4      =    D0W
                                                      , QW
                                                         4 =         D0Z
                                                                               − 1, QZ4 =   D0W
                                                                                                  H0W − 1.
It easy to remark that
Remark 2.
  1. If R0 < 1, then the point E1 does not exist and E1 = Ef when R0 = 1.
  2. If H0Z < 1, then E2 does not exists and E2 = E1 when H0Z = 1.
  3. If H0W < 1, then E3 does not exists and E3 = E1 when H0W = 1.
                          D0Z
  4. If D0W < D0Z or      D0W
                                 H0W < 1, then E4 does not exists. Moreover E4 = E2
                                                               D0Z
     when D0W = D0Z and E4 = E3 when                           D0W
                                                                     H0W = 1.
   The number D0W represents the basic defence number by antibody response,
 Z
D0 represents the basic defence number by CTL response.
H0W is the half harmonic mean of R0 and D0W and H0Z is the half harmonic
mean of R0 and D0Z .
We put
                                                          H0W D0Z
                                           H0W,Z =         D0W
4004                                                                 Adil Meskaf et al.
We remark that H0W = H0W,W and H0Z = H0Z,Z . The importance of these
parameters is related to the following result:
Proposition 3.
  1. If R0 ≤ 1, then the point E0 is globally asymptotically stable.
  2. If R0 > 1, H0W ≤ 1 and H0Z ≤ 1, then E1 is globally asymptotically
     stable.
  3. If H0Z > 1 and D0Z > D0W , then the point E2 is globally asymptotically
     stable.
  4. If H0W > 1 and H0W,Z ≤ 1, then the point E3 is globally asymptotically
     stable.
  5. If D0W > D0Z and H0W,Z > 1, then the point E4 is globally asymptotically
     stable.
  Proof. For the proof, we will use the same techniques given in [3, 7, 10].
We consider the following Lyapunov function defined in R5+ by:
                                X       X           Y      Y
           V (X, Y, V, W, Z) = x∗ (
                                  ∗
                                    − ln ∗ ) + Y ∗ ( ∗ − ln ∗ ) +
                                X       X           Y      Y
  β(1 − u1 )X ∗ ∗ V       V      q ∗ W          W       p ∗ Z     Z
            ∗
               [V ( ∗ − ln ∗ ) + W ( ∗ − ln ∗ )] + Z ( ∗ − ln ∗ ),
    u + qW         V      V      g     W        W       c    Z    Z
   where E ∗ = (X ∗ , Y ∗ , V ∗ , W ∗ , Z ∗ ) is an equilibrium of the system.
   It easy to verifies that
                                        R0 QXi    QVi     QW
                                                           i       QZi
 V̇ (X, Y, V, W, Z) = λ[1 + QX    Y
                             i + Qi +           (      +      ) +      ] − (dX +
                                       1 + QW i   R0      D0W      D0Z
  λ2 X      β(1 − u1 )λXV Y       λ(1 − u2 )kY QX  i Qi
                                                        V
                                                                  R0 QX i
     Qi ) −                 Qi −                          +  ay(           −1−
  dX              ay                   δv       1 + QW  i        1 +  Q  W
                                                                         i
           W qλ QX i           R0      pλz Y          1      pλz Y          1
   QZi ) +           W
                       (QVi − W ) +        (Qi − Z ) +           (Qi − Z ).
            δ 1 + Qi           D0       a           D0        a            D0
For i = 0 we have
                            λ2                   λqW R0   pλZ 1
        V̇ = 2λ − (dX +        ) + aY (R0 − 1) −      W
                                                        −        .
                            dX                     δ D0    a D0Z
Since
                                         λ2
                                  dX +      ≥ 2λ,
                                         dX
Global analysis of a HCV model with CTL, antibody responses and therapy 4005
then V̇ < 0 and E0 is globally asymptotically stable, if R0 ≤ 1.
For i = 1 we have that
               1                 λ2       β(1 − u1 )λXV         1     λk(1 − u2 )y       1
V̇    = λ(3 −     ) − (dX +           )−                 (1 −     )−               (1 −     )
              R0               R0 dX            aY             R0         uV             R0
          λqW          1       pλZ         1
        +      (1 − W ) +           (1 − Z )
            δ        H0          a        H0
                 1       2                λ2         λ2        1      β(1 − u1 )λXV         1
      = λ[3(1 −     )+      ] − (dX + 2        )−        (1 −     )−                  (1 −    )
                R0       R0             R0 dX      R0 dX       R0           ay             R0
          λk(1 − u2 )Y         1      λqW         1      pλZ        1
        −               (1 −      )+        (1 − W ) +        (1 − Z ).
               δV             R0        δ        H0        a       H0
Using the arithmetic-geometric inequality, if R0 > 1, we have
         2                     β(1−u1 )λXV                      λk(1−u2 )Y
     − R0λdX (1 −   1
                    R0
                       )   −       ay
                                              (1 −   1
                                                     R0
                                                        )   −       δV
                                                                             (1 −   1
                                                                                    R0
                                                                                       )   ≤ −3λ(1 −   1
                                                                                                       R0
                                                                                                          ).
Since
                                                       λ2           2λ
                                              dX +   R02 dX
                                                                ≥   R0
                                                                       ,
then V̇ < 0 and E1 is globally asymptotically stable, if R0 > 1, H0W ≤ 1 and
H0Z ≤ 1.
For i = 2 we have
               H0Z             λ2 H0Z     β(1 − u1 )λXV 1      λk(1 − u2 )Y H0Z
V̇    = λ(3 −      ) − (dX +          )−                     −
                R0             dX R0           aY        D0Z       δV       D0Z
          λqW z 1            1
        +       H0 ( Z − W )
            δ        D0     D0
              Z        Z
           H         H             λ2 H0Z 2      λ2 H0Z      HZ     β(1 − u1 )λXV 1
      = λ(3 0Z + 2 0 ) − [dX +         (   ) ]−         (1 − 0 ) −
           D0        R0            dX R0         dX R0       R0            aY    D0Z
          λk(1 − u2 )Y H0Z λqW Z 1              1
        −                 Z
                             +      H0 ( Z − W ).
                δV       D0      δ       D0    D0
      Using the arithmetico-geometric inequality, we have
               λ2   H0Z          H0Z         β(1−u1 )λXV 1           λk(1−u2 )Y H0Z            HZ
             − dX   R0
                        (1   −   R0
                                     )   −       aY     D0Z
                                                                 −       δV     D0Z
                                                                                      ≤ −3λ D0Z .
                                                                                                0
Since
                                                       Z               HZ
                                                λ2 H0 2
                                         dx +     ( )
                                                dX R0
                                                                ≥ 2λ R00 ,
4006                                                                                Adil Meskaf et al.
    then V̇ < 0 and E2 is globally asymptotically stable, if H0Z > 1 and D0Z >
D0W .
For i = 3 we have
         H0W      H0W            λ2 H0W 2      λ2 H0W       H0W     β(1 − u1 )λXV H0W
V̇ = λ(3 W + 2        ) − [dX +      (    ) ]−        (1 −       )−
         D0       R0             dX R0         dx R0         R0           ay      D0W
      λk(1 − u2 )Y 1      λpZ
   −                 W
                        +    Z
                               (H0W,Z − 1).
           δV     D0      aD0
Using the arithmetico-geometric inequality, we have
          λ 2   H0W          H0W        β(1−u1 )λXV H0W        λk(1−u2 )Y 1              HW
        − dX    R0
                      (1 −   R0
                                   )−       aY      D0W
                                                           −       δV    D0Z
                                                                                  ≤ −3λ D0W .
                                                                                          0
Since
                                                   W             H0W
                                            λ2 H 0
                                    dX +      (
                                            dX R0
                                                       )2 ≥ 2λ   R0
                                                                       ,
   then V̇ < 0 and E3 is globally asymptotically stable, if H0W ≥ 1 and
H0W,Z < 1.
For i = 4 we have
           H0W            λ2 H0W    β(1 − u1 )λXV 1      λk(1 − u2 )Y H0W,Z
V̇ = λ(3 −     ) − (dX +         )−                    −                    ,
           R0            dX R0           aY        D0Z       δV        D0Z
           HW            λ2 H0W 2     λ2 H0W       HW     β(1 − u1 )λXV 1
   = λ(3 − 0 ) − [dX +       (   ) ]−          (1 − 0 ) −
           R0            dX R0        dX R0         R0          aY        D0Z
    λk(1 − u2 )Y H0W,Z
  −                    .
         δV       D0Z
Using the arithmetico-geometric inequality, we have
                                                                         W,Z
          λ2    H0W          H0W        β(1−u1 )λXV 1        λk(1−u2 )Y H0               HW
        − dX    R0
                      (1 −   R0
                                   )−       ay     D0Z
                                                         −       δV     D0W
                                                                                  ≤ −3λ D0W .
                                                                                           0
Since
                                                   W             H0W
                                            λ2 H 0
                                    dX +      (
                                            dX R0
                                                       )2 ≥ 2λ   R0
                                                                       ,
   then V̇ ≤ 0.
The equality holds if and only if
                                                       k(1−u2 ) D0Z        V∗
                             X = X ∗ and       V
                                               Y
                                                   =      δ     D0W
                                                                       =   Y∗
                                                                              .
Let
                S = {(X, Y, V, W, Z) ∈ IR5+ : V̇ (X, Y, V, W, Z) = 0}.
The trajectory (X(t), Y (t), V (t), W (t), Z(t)) ∈ S implies that
                        Y = Y ∗ , V = V ∗ , W = W ∗ and Z = Z ∗ .
From LaSalle’s invariance principle [?], we conclude that E4 is globally asymp-
totically stable, if D0W > D0Z and H0W,Z > 1.
Global analysis of a HCV model with CTL, antibody responses and therapy 4007
Figure 1: The basic reproduction number R0 as function of the drug efficacy
θ for λ = 2.105 , β = 2.10−7 , k = 20, d = 0.1, a = 0.5 and δ = 4.
4    Discussion and conclusion
In this work, we gave the global analysis of a HCV with CTL, antibody re-
sponses and therapy The disease free equilibrium is globally asymptotically
stable if the basic infection reproduction number satisfies R0 ≤ 1. For R0 > 1,
the global stability of the four endemic equilibrium points depends on both
the basic defence rate by antibody response and the basic defence rate by
CTL response. In addition, the goal of the therapy is to better control the
concentrations of the virus and infected cells in order to reduce the value of
the number of basic reproduction to a number below one. Indeed, if we put
θ = u1 + u2 − u1 u2 which represents the combined efficacy of the two drugs,
we will have 1 − θ = (1 − u1 )(1 − u2 ) which means that each drug acts inde-
pendently. Hence, R0 becomes
                                     λβ(1 − θ)k
                              R0 =              .
                                        daδ
Then from the above formula of R0 , we see that R0 can be decreased by
increasing the efficacy of therapy, i.e. increasing u1 and u2 (see Fig. 1).
4008                                                          Adil Meskaf et al.
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Received: April 27, 2015; Published: May 21, 2015