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ISSN: 2278 – 1323
                                            International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                Volume 1, Issue 2, April 2012


       The dynamics of disease transmission in a Prey Predator System with
                                         harvesting of prey
                                       , Kul Bhushan Agnihotri*


                            Department of Applied Sciences and Humanties
         Shaheed Bhagat Singh College of Engg & Tech Ferozepur-152004, Punjab, India
                                           Sunita Gakkhar **


                        Department of Mathematics, IIT Roorkee, Roorkee, India
 Abstract: In this present work on predator-prey system, a disease transmission model,
 incorporating provisions for harvesting of prey have been discussed and analyzed. The disease
 spread is from infected prey to predator species. The SI models are considered for both the
 species. Conditions are derived for existence and stability of disease free equilibrium state of
 the system. The effect of harvesting of prey has been analyzed from point view of the stability
 of system. The epidemiological threshold R0 and R1 quantities have been obtained using next

 generation approach for the model system. Conditions for endemic disease in prey species are
 discussed. This study also considers the impact of disease in prey on the extinction aspect of the
 predator. Numerical and computer simulations of the model have been done.
Mathematics Subject Classification (2000) 35B35 - 92C05 - 92D30 -92D40
         Keywords: Predator, prey, Equilibrium point, carrying capacity, Basic reproduction number,
Stability, Harvesting

    1. Introduction:
       Predator-prey interactions give regulatory system for the advancement of biological
species. in natural ecosystem. Prey predator interactions and disease in the system affects each
other [1, 3, 5, 7, 8-10, and 17]. Some previous studies of infectious diseases in animal
populations were focused on the effects of disease-induced mortality or disease-reduced
reproduction in the regulation of populations in their natural habitats [3, 7, 8, 17 and 18].
Reduced population sizes and destabilization of equilibrium into oscillations are caused by the
presence of infectious disease in one or both of the populations.
       The fact that predators take a disproportionate number of infected preys has been
confirmed by earlier studies [8, 11 and 17]. Infected prey is more exposed to predation on

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ISSN: 2278 – 1323
                                           International Journal of Advanced Research in Computer Engineering & Technology
                                                                                               Volume 1, Issue 2, April 2012


account of the fact that the disease may weaken their ability to protect themselves and expose
them to predators [1]. This increased vulnerability of infected prey may lead to persistence of the
predator (which would otherwise be starved and become extinct). Further, predation of the
infected prey may lead to the disappearance of disease which may otherwise be endemic in prey
population [3]. Together with no reproduction in infected prey, as predation on infected prey
increases, the infection tends to destabilize prey-predator interactions [17].
      Most of the eco-epidemiological studies are restricted to the situations where only prey
species can get infection. Few investigations [4, 11, 19-21] consider the spread of disease from
prey to predator through predation of infected prey. For the purpose of eliminating either the
disease from predator- prey system or eliminating the menace of the predator by controlling
disease in prey, a simplified eco- epidemiological four species prey predator SI model [4] is
shown to be useful.
        Exploitation of biological resources as practiced in fishery, and forestry has strong impact
on dynamic evolution of biological population. The over exploitation of resources may lead to
extinction of species which adversely affects the ecosystem. However, reasonable and controlled
harvesting is beneficial from economical and ecological point of view. The research on
harvesting in predator-prey systems has been of interest to economists, ecologists and natural
resource management for some time now. Very few has explicitly put a harvested parameter in a
predator–prey–parasite model and studied its effect on the system. Here we study the role of
harvesting in an eco-epidemiological system where the susceptible and infected prey are
subjected to combined harvesting.
      In this present work on predator-prey system, a disease transmission model, incorporating
provisions for harvesting of prey have been proposed and studied. In the model, the disease is
spreading from infected prey to susceptible prey and consequently to the predator species via
predation related activities: capturing, handling and eating the infected prey. Both, the prey and
the predator species are compartmentalized into susceptible and infected classes. Recovery from
disease is not considered for both prey and the predator species. Consequently, SI model is
considered for both the species.
    2. Mathematical Analysis
        Consider an eco-epidemiological system comprising of four populations, namely, the
susceptible prey ( S1 ), infected prey ( I1 ), susceptible predator ( S 2 ) and infective predator ( I 2 )

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ISSN: 2278 – 1323
                                              International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                  Volume 1, Issue 2, April 2012


such that N1  t   S1 (t )  I1 (t ) and N 2  t   S2 (t )  I 2 (t ) . An SI type eco-epidemiological model

for prey predator dynamics is presented under following assumptions:
        Only susceptible prey is capable of reproducing logistically. While susceptible prey can
easily escape the predation, the infected prey are weakened due to disease and become easier to
catch. The infected prey and predator do not reproduce but still continue to consume resources.
The susceptible predator gets food from infected prey for its survival. It may become infected
due to interaction with infected prey. Mortality rate of infected predator is higher than that of
susceptible predator. It is also assumed that the disease does not affect the hunting ability of
infected predator. Further, all the predators who predate the infected prey become infected. Let
e1 be the harvesting rate of susceptible prey and e2 be the harvesting rate of infected prey. Since

it is easy to catch infected prey as compare to susceptible prey, therefore e1  e2 .
        Accordingly, the following mathematical model is obtained under the above assumptions:
                 dS1          S I 
                       rS1 1- 1 1  - a1S1 ( S2  I 2 ) - c1S1I1  e1S1
                 dt                 K1 
                 dI1
                       c1S1 I1 - a2 I1 ( S2  I 2 ) - d1 I1  e2 I1
                 dt
                 dS2
                       -a2 S2 I1  (-d 2  ka1S1 ) S2
                  dt
                 dI 2
                       a2 S2 I1 - d3 I 2
                 dt                                                                                      (1)
       where
                 a1  Predation rate on the susceptible prey (hectare per individual day-1)

                 a2  Predation rate on the infective prey (hectare per individual day-1)

                 k  Feeding efficiency of predator (per individual day-1)
                  r  Intrinsic growth rate constant of susceptible prey (day-1)
                 K1  Carrying capacity of environment with respect to prey species

                       (Individual ha-1)
                  c1  Rate of force of infection (hectare per individual day-1)

                 d1  Net death rate of prey (Natural death + death due to infection) (day-1)

                 d 2  Natural death rate of susceptible predator (day-1)


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                                                          International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                              Volume 1, Issue 2, April 2012


                    d3  Net death rate of infected predator (day )
                                                                 -1


According            to          the               assumptions a2  a1 , d3  d2                 and            e2  e1 , k  1. Also,

S1 (0)  0, S2 (0)  0, I1 (0)  0 and I 2 (0)  0 .

    3. Mathematical Analysis

Theorem 1 All the solutions of the system (1) which initiate in  4 are uniformly bounded.
                                                                  


Proof: By theorems of Nagumo [13] , it can be easily proved that S1 , I1 , S 2 and I 2 remain

positive. Let W1  S1  I1

From (1), the following can be easily obtained:
               d ( S1  I1 )        S 
                              rS1 1- 1   e1S1 - d1I1  e2 I1
                    dt              K1 
               d (S1  I1 )                rS 2
                             (r  e1 )S1 - 1 - (d1  e2 ) I1
                   dt                       K1
For arbitrarily chosen 1 , this simplifies to

d ( S1  I1 )                                       rS 2
               1 ( S1  I1 )  (r  e1  1 ) S1 - 1 - (d1  e2  1 ) I1
     dt                                              K1
dW1               K1 (r  e1  1 ) 2
                                          r  2                  K1         K12 (r  e1  1 ) 2 
       1W1                           S1  (r  e1  1 ) S1                                 - (d1  e2  1 ) I1
 dt                        4r            K1                      r                4r 2          
            K (r  e1  1 )2 r 
                                                                               2
dW1                                                 K 
     1W1  1                 S1  (r  e1  1 ) 1  - (d1  e2  1 ) I1
 dt               4r          K1                   2r 

Choosing 1  d1  e2 and applying the results of Birkhoff and Rota [6], yields

                                              L1                                                       K1 (r  e1  1 )2
               0  W1 ( S1 (t ), I1 (t ))         (1  e 1t )  W1 ( S1 (0), I1 (0))e 1t ; L1 
                                              1                                                              4r
As t   , it gives
                                 L1
               0  S1  I1           ( K ) ,
                                1
            W1  S1  I1 is bounded

From positivity of S1 and I1 ,

               0  S1  K ;0  I1  K .


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ISSN: 2278 – 1323
                                                        International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                            Volume 1, Issue 2, April 2012


Similarly, defining another positive definite function W as
              W  S1  I1  S2  I 2

Proceeding in the similar manner and choosing   min(d1  e2 , d 2 , d3 ) yields

                                               L1 (r   )
              0  W ( S1 , I1 , S 2 .I 2 )                  (1  e t )  W ( S1 (0), I1 (0), S 2 (0), I 2 (0))e t
                                                 1
As t   , it gives
                          K (r   )                               (r   )
              0 W                      L , where L 
                                                                    
             W      S1  I1  S2  I 2 is bounded.
                                                              4
Hence all solutions of (1) that initiate in                     are confined in the region

                   
              B  ( S1 , I1 , S2 , I 2 )   n : Si  L; I i  L; i  1, 2
                                                                                 
   4.     Equilibrium points:
        The following equilibrium points exist for the system (1):
             a) The trivial equilibrium point E0 (0,0,0,0)

             b) The axial equilibrium point E1 ( S1 , 0, 0, 0) ,

                               K (r  e1 ) 
                   Where S1   1            always exist provided
                                   r       
                             r  e1 .                                                                                (2)

             c) The planar equilibrium point E2 ( S1' , I1' ,0,0) in S1  I1 plane is

                  obtained as
                                     d1  e2 ' c1K1 (r  e1 )  (d1  e2 )r
                             S1'           , I1                             ,
                                        c1             c1 (c1K1  r )
         The existence of this equilibrium point is possible provided
                  c1K1 (r  e1 )  (d1  e2 )r  0                                                                       (3)

        In this case, the predator species is eliminated and the disease persists in the prey species.
        Harvesting of susceptible and infected prey will reduce the possibility of existence of




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ISSN: 2278 – 1323
                                                     International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                         Volume 1, Issue 2, April 2012


      E2 ( S1' , I1' ,0,0). If it exist then number of susceptible prey will increase but number of

      infected prey will decrease due to harvesting of susceptible and infected prey.
                                                        ˆ      ˆ
      Another disease free planar equilibrium point E3 (S1 ,0, S2 ,0) on S1  S2 plane exists

      provided
                  ka1K1 (r  e1 )  rd2  0                                                                     (4)
      where

              ˆ   d       ˆ ka K (r  e )  rd 2 ,
              S1  2 and, S2  1 1 2 1
                  ka1             ka1 K1
      It has been also observed that even if the feeding efficiency k of predator is high enough
                  d2                                                  ˆ      ˆ
      that K1        , even then the disease free equilibrium in E3 (S1 ,0, S2 ,0) may not exist with
                  ka1
      harvesting of susceptible prey. If it exists then number of susceptible prey will remain
      same but number of susceptible predator will decrease due to removal of susceptible prey.
              d)             For non-zero equilibrium point E* (S1* , I1* , S1* , I1* ) of the system (1)

      is given by
                                                                     ˆ
                          (r  e1 )a2 K1  a1c1K1S1'  (r  c1K1 )ka1S1
                  S1* 
                                   r (a2  ka1 )  a1c1K1 (1  k )
                                     ˆ
                          ka1 (S1*  S1 )
                  I1*                    ,                 S1*  I1*  K1
                                a2

                              c1d3 ( S1*  S1' )
                  S2 
                   *
                                                    ,
                                           ˆ
                          a2 (d3  (S1*  S1 )ka1 )
                                      ˆ *
                          ka1 ( S1*  S1 )S2
                  I2 
                   *

                                   d3

       Accordingly, E * (S * , I * , S * , I * ) exists provided

                  S1*  max  S1' , S1   S , r  e1
                                    ˆ                                                                           (5)

      The Basic Reproduction Number is defined as the average number of secondary infections
when one infective is introduced into a completely susceptible host population. It is also called
the basic reproduction ratio or basic reproductive rate. Using next generation approach [2, 15 and
16], the epidemiological threshold quantities for the system (1) are obtained as

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ISSN: 2278 – 1323
                                                    International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                        Volume 1, Issue 2, April 2012


                     c1K1 (r  e1 )                ˆ
                                                c1S1
              R0                   , R1                                                                       (6)
                      r (d1  e2 )                      ˆ
                                           d1  e2  a2 S2

        Here, R0 is the basic reproduction number for isolated prey population and R1 is the basic

reproduction in the prey population when both prey and predator are present in the system. The
greater vulnerability of prey will reduce R1 . Harvesting of infected prey (e2 ) will reduce both

 R1 and R2 . Also by simplification it can be proved that R0  R1

   5.   Local Stability Analysis
The variational matrix V of given system (1) is given by


                     2rS1                            rI1               rS                                                   
                     r  K - a1 (S2  I 2 ) - c1I1 - K  e1          - 1 - c1S1
                                                                        K1
                                                                                                      -a1S1           -a1S1 
                          1                            1                                                                    
                 V                 c1I1                    c1S1 - d1 - a2 (S2  I 2 )  e2          -a2 I1          -a2 I1 
                                                                                                                            
                                  ka1S2                                 -a2 S2              -a2 I1  (-d 2  ka1S1 ) 0 
                                                                                                                      -d 3 
                                     0                                   a2 S2                        a2 I1                 
The following theorem is direct consequences of linear stability analysis of the system (1) about
E0 and E1 .

Theorem 2 The trivial equilibrium point E0 (0,0,0,0) is locally asymptotically stable provided

                 r  e1
                                                                                                                (7)
Theorem 3 The axial equilibrium E1 ( S1 , 0, 0, 0) is locally asymptotically stable provided

                       ˆ
         S1  min S1' , S1                                                                                     (8)

The equilibrium E1 ( S1 , 0, 0, 0) is unstable when

                                            
                                      S1  min  S1' , S1  , 
                                                       ˆ                                                       (9)

It can be concluded from (8) that E1 ( S1 , 0, 0, 0) may be stable for those parametric values for

which it was not stable without harvesting of prey. So harvesting of susceptible and infected prey
has positive effect on the stability of E1 ( S1 , 0, 0, 0).

Also from (8) it may be noticed that when E1 ( S1 , 0, 0, 0) is locally asymptotically stable,



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ISSN: 2278 – 1323
                                                 International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                     Volume 1, Issue 2, April 2012


                         d1  e2         d
                  S1            and S1  2 ,
                            c1           ka1

                            (d1  e2 )r               rd 2
                   K1                  and K1                or
                            c1 (r  e1 )          ka1 (r  e1 )
                                          rd 2
                  R0  1 and K1 
                                      ka1 (r  e1 )
                                                                                ˆ      ˆ
which violate existence conditions (3) and (4) of E2 ( S1' , I1' ,0,0) and E3 ( S1 ,0, S2 ,0) respectively.

So, when E1 ( S1 , 0, 0, 0) is locally asymptotically stable then E0 (0,0,0,0), E2 ( S1' , I1' ,0,0) and

     ˆ      ˆ
E3 ( S1 ,0, S2 ,0) do not exist.

        When the perturbations are confined in S1  I1 plane only, then the equilibrium point

E1 ( S1 , 0, 0, 0) is locally asymptotically stable for R0  1 . However in the presence of predator

population the stability depends upon the dynamics of predator also as is evident from (8). In
fact, when the feeding efficiency of predator is sufficiently low then the disease will die out from
both the prey and predator under condition (8) and the equilibrium point E1 ( S1 , 0, 0, 0) is locally

asymptotically stable. In other words, when the feeding efficiency is sufficiently low and the
basic reproduction number R0 in prey population is below the threshold then predator population
become extinct and disease dies out from the prey population.
Theorem 4. If R0  1 , then E2 (S1' , I1' ,0,0) locally asymptotically stable provided

                  ka1S1'  a2 I1'  d2  0                                                                  (10)

Proof: From variational matrix V, the characteristic equation about E2 (S1' , I1' ,0,0) is obtained as

                2 rS1'
                                   rS '      
                       c1 I1'  1  c1S1'   (a2 I1'  ka1S1'  d 2   ) (d3   )  0
               
                    K1             K1        
The quadratic factor gives two eigen values with negative real parts
. Therefore, the system around E2 (S1' , I1' ,0,0) is locally asymptotically stable provided (10) is

satisfied. 
If the basic reproduction number R0 in the prey population is above the threshold, the disease in
prey population approaches to endemic level and predator population becomes extinct due to
(10).

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ISSN: 2278 – 1323
                                                   International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                       Volume 1, Issue 2, April 2012


Harvesting of susceptible and infected prey has negative effect on the stability of E2 (S1' , I1' ,0,0).

The condition of instability of E2 (S1' , I1' ,0,0) if it exists, is given by

                 ka1S1'  a2 I1'  d2  0                                                                        (11)
                                                   ˆ      ˆ
Theorem 5. The disease free equilibrium state E3 ( S1 ,0, S2 ,0) , if it exists, is locally
                                                                               ,

asymptotically stable provided R1  1 .
                                                                         ˆ      ˆ
Proof: From variational matrix V, the characteristic equation about E3 ( S1 ,0, S2 ,0) is
                     ˆ
                    rS1
           ( 2                 ˆ ˆ      ˆ       ˆ
                          ka12 S1S2 )(c1S1  a2 S2  d1  e2   )(d3   )  0
                    K1
Since the quadratic factor always yield eigen values with negative real parts, the condition for
stability is
                    ˆ       ˆ
                  c1S1  a2 S2  d1  e2  0
Its simplification gives
                   R1  1                                                                                      (12)

This completes the proof. 
      When the basic reproduction number R1 is below the threshold, then the disease dies out
                                                     ˆ      ˆ
from both the species and the equilibrium point E3 ( S1 ,0, S2 ,0) is stabilized. Rewriting

stability condition gives the critical value of e2 for which the disease free equilibrium state is
locally asymptotically stable:
                           ra  ˆ a                     ˆ d
                 e2   c1  2  S1  2 (r  e1 )  d1 , S1  2
                           K1a1    a1                      ka1
                                                                                                            (13)
The greater vulnerability of prey to predation may be responsible for persistence of disease free
prey predator population.
      By simplifying above condition for stability it has been observed that harvesting of
                                                                  ˆ      ˆ
infected prey may improve the stability of equilibrium point E3 ( S1 ,0, S2 ,0) where as it become
less stable with harvesting of susceptible prey. Thus with an appropriate harvesting of
                                                                   ˆ      ˆ
susceptible and infected prey, disease free equilibrium point E3 ( S1 ,0, S2 ,0) can be maintained at

desired level.

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                                                 International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                     Volume 1, Issue 2, April 2012


                                                  ˆ      ˆ
          The disease free equilibrium state E3 ( S1 ,0, S2 ,0) if it exist, is unstable if
                    ˆ       ˆ
                  c1S1  a2 S2  d1  e2  0                                                                (14)

It is observed that E2 (S1' , I1' ,0,0) , if it exists, is locally asymptotically stable provided
     ˆ      ˆ
E3 ( S1 ,0, S2 ,0) is unstable and vice-versa.
However, it is possible for some choice of parameters that both E2 ( S1, I1, 0, 0) and
     ˆ      ˆ
 E3 (S1 ,0, S2 ,0) exist and locally stable.
                                                                ˆ      ˆ
It is also observed that when both E2 ( S1, I1, 0, 0) and E3 (S1 ,0, S2 ,0) are stable then non-zero

equilibrium point E* (S1* , I1* , S2* , I 2* ) always exist.

Theorem 6. The non-zero equilibrium point E* (S1* , I1* , S1* , I1* ) , if exists, is a saddle point.

Proof:      The characteristic equation about E* is obtained as
                 4  A0 3  A1 2  A2  A3  0                                                             (15)

Where
                                                                   r 
                 A3  a2 (d3  a2 I1* ) (k  1)a1c1   ka1  a2   I1*S1*S 2
                                                                               *

                                                                   K1 

As the constant term A3 is always negative, at least one eigenvalue of the equation (15) will be

positive, therefore E* (S1* , I1* , S2 , I 2 ) is not locally asymptotically stable.
                                     * *



It is either unstable or a saddle point.        □
     6.     Numerical simulations
Numerical simulations have been carried out to investigate dynamics of the proposed model.
Computer simulations have been performed on MATLAB for different set of parameters.
Consider the following set of parametric values:
                 r  0.1, K1  50, e1  0.03, e2  0.05, d1  0.7, d 2  0.6,
                                                                                                            (16)
               d3  0.7, c1  0.01, a1  0.8, a2  0.9, k  0.012

The system (1) has equilibrium point E1 (35, 0, 0, 0) for the data set (16). It is locally

asymptotically stable by the computed value of R0 is 0.4667  1 and the value of feeding

efficiency k of predator population is sufficiently low and the condition (8) is satisfied. The
solution trajectories in phase space S1  I1  S2 are drawn in Fig. 1 for different initial values. All

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                                                                   International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                                       Volume 1, Issue 2, April 2012


the                            solution                                   trajectories                             to                        tend
to E1 (35, 0, 0, 0).



                                                       D
                20

                15                                                                                         A=( 1, 10, 10, 1 )

                10                                                                                         B=( 20, 0, 10, 0 )
           S2




                                      A                                                                    C=( 20, 10, 0, 0 )
                   5
                                                                                      B
                                                                                                           D=( 20, 20, 20, 20 )
                 0
                20                                                       C                            E1 E =( 35, 0, 0, 0 )
                                                                                                          1
                         15
                                10                                                                   30
                                          5                                               20
                                                                          10
                                 I1                0       0                     S1


       Fig 1: Phase plot depicting the stability of equilibrium point E1 in phase space S1 - I1 - S2 for data-set (16)

Now consider following set of data
                r  0.02, K1  100, e1  0.021, e2  0.03, d1  0.01, d 2  0.11,
                                                                                                                              (17)
                d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33

For above set of data, the equilibrium point E0 (0, 0, 0, 0) is locally asymptotically stable as r  e1

(see        Fig.         2)          and           all          other            equilibrium              points         do      not        exist.



               20                              D

               15
                                                                                                    A=( 1, 10, 10, 1 )
               10
          S2




                                                                                                    B=( 20, 0, 10, 0 )
                5
                                 A                                                                  C=( 20, 10, 0, 0 )
                0                                                            B                      D=( 20, 20, 20, 20 )
               20                                              C
                    15                                                                              E0=( 0, 0, 0, 0 )
                         10
                                5                                                              30
                                                                             20
                          I1          0                        10
                                           0
                                          E0                        S1




                                                   All Rights Reserved © 2012 IJARCET                                                           11
ISSN: 2278 – 1323
                                                    International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                        Volume 1, Issue 2, April 2012


      Fig 2: Phase plot depicting the stability of equilibrium point E1 in phase space S1 - I1 - S2 for data set 17

        For the following data set of parameters, E2 is stable and E3 is unstable:

              r  0.02, K1  100, e1  0.01, e2  0.03, d1  0.01, d 2  0.11,
                                                                                                                         (18)
              d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33

The equilibrium point E1 (50, 0, 0, 0) is unstable as condition (8) is not satisfied and both the

planar equilibrium points E2 (20, 2.7273, 0, 0) and E3 (33.3333, 0, 0.3333, 0) exists condition

(3) and (4) are satisfied respectively. The equilibrium point E3 (33.3333, 0, 0.3333, 0) is found to

be unstable as it satisfies the condition (14). The equilibrium point E2 (20, 2.7273, 0, 0) is found

to be locally asymptotically stable as condition (10) is satisfied. The solution trajectories in phase
space S1  I1  S2 are drawn in Fig. 4 for different initial values. All these trajectories converge

to E2 (20, 2.7273, 0, 0) .        Starting        with        initial    value       in      the      neighborhood           of      the

point E3 (33.3333, 0, 0.3333, 0) , the solution trajectory approaches to the equilibrium point

E2 (20, 2.7273, 0, 0). This confirms the instability of E3 .



              20                          D
                                                                                             E2=(20, 2.7273, 0, 0)
              15
                                                                                               A=(0.1, 0.1, 0.1,0.1)
              10
         S2




               5                                                                               B=(50, 0.1, 0.1, 0.1)

               0                                                                               C=(33.33,0.1,0.33,0.1)
              20
                   15                             E2                                      B D=(20, 20, 20, 20)
                                                                           C
                        10                                                                     50
                                         A                                          40
                              5                                            30
                                                                   20
                        I1          0                    10
                                              0
                                                                S1


     Fig. 3: Phase plot depicting the stability of       E2    and instability of   E3 in   S1  I1  S 2   space for dataset (18)




                                         All Rights Reserved © 2012 IJARCET                                                          12
ISSN: 2278 – 1323
                                                  International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                      Volume 1, Issue 2, April 2012


The following data is selected for which all the equilibrium points exist:
             r  0.02, K1  100, e1  0.01, e2  0.068, d1  0.01, d 2  0.11,
                                                                                                               (19)
             d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33

In this case, the equilibrium point E1 (50, 0, 0, 0) is unstable. It is observed that both the

equilibrium points E2 (39, 1, 0, 0) and E3 (33.3333, 0, 0.3333, 0) are locally asymptotically stable.

The point E2 (39, 1, 0, 0) is stable since ka1S1'  d3 I1'  d2  0.0013  0 and R0  1.2821  1 . Also,

E3 (33.3333, 0, 0.3333, 0)        is locally asymptotically stable as R1  0.7874  1 . Both the

equilibrium points have their own domains of attractions. Trajectories with different initial
conditions converge to different equilibrium points (See Fig. 4).
        The instability of non-zero equilibrium point E* (39.0915,0.9501,0.0081,0.0010) can be
seen from Fig. 4. It is also noticed that when even a very small perturbation is taken from
E* (39.0915,0.9501,0.0081,0.0010)            to D(40, 0.9501, 0.0081, 0.0010) , along                     S1 direction, the

trajectory   converges      to E2 (39, 1, 0, 0) .        Whereas,          when       the      perturbation         is     taken

to E (39.0915,1, 0.0081, 0.0010) ,          the          trajectory          of        the         system           converges
to E3 (33.3333, 0, 0.3333, 0) .

         A=(0.1, 0.1, 0.1,0.1) B=(50, 0.1, 0.1, 0.1) C=(1, 1, 1, 1) D=(40, 0.9501, 0.0081, 0.0010)

                                                                                    E=(39.0915, 1, 0.0081,0.00100)
                                                                                                             E2=(39,1, 0, 0)
                      1                                                                        E3=(33.3333,0.3333,0,0)
                                        E3
                                                                             A
                S2




                     0.5

                                                                                              C
                      0
                      0      B


                            0.5
                                                       D                                           0
                             I1                          E                               10
                                                        E 2                    20
                                        1                            30
                                                           40
                                                  50                S1


        Fig 4: Phase plot depicting the stable behaviour of E2 , E3 in S1  I1  S2 space for dataset (19)




                                      All Rights Reserved © 2012 IJARCET                                                       13
ISSN: 2278 – 1323
                                                    International Journal of Advanced Research in Computer Engineering & Technology
                                                                                                        Volume 1, Issue 2, April 2012


           Now, consider the following data set where E3 is stable and E2 unstable:

                 r  0.02, K1  100, e1  0.01, e2  0.069, d1  0.01, d 2  0.11,
                                                                                                                   (20)
                 d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33

                                                                             d2              (d1  e2 )
As S1 ( 50) is greater than computed value 33.3333 of                           and 39.5 of            in this case,
                                                                             ka1                 c1

the equilibrium point E1 (50, 0, 0, 0) is unstable and system (1) has two planar equilibrium points,

say        E2 (39.5, 0.9545, 0, 0)      and       E3 (33.3333, 0, 0.3333, 0) .                  The           equilibrium     point

E3 (33.3333, 0, 0.3333, 0) is found to be stable as it satisfies the condition (12). The equilibrium

point E2 (39.5, 0.9545, 0, 0) is found to be unstable as it satisfies the condition (11). The solution
trajectories in phase space S1 - I1 - S2 are drawn in Fig. 5 for different initial values. All these
trajectories approach to E3 (33.3333, 0, 0.3333, 0) . Convergence of solution trajectory to

equilibrium E3 (33.3333, 0, 0.3333, 0) with initial value near E2 (39.5, 0.9545, 0, 0) also confirms

the instability of E2 (39.5, 0.9545, 0, 0) .

 A=(0.1, 0.1, 0.1,0.1)          B=(50, 0.1, 0.1, 0.1)         C=(1, 1, 1, 1)        D=(39.5, 0.9545, 0.1, 0.1)
                                                                                    E3=(33.3333, 0, 0.3333,0)
           1.5


            1
                                                                                                               C
      S2




                                   E3
           0.5                                                           A

                    B
            0
            0
                                                                D                                        10        0
                           0.5                                                             20
                                                                              30
                                                1                   40
                           I1                          50
                                                                             S1


       Fig. 5: Phase plot depicting the stability of   E3   and instability of   E2 in   S1  I1  S 2   space for dataset (20)




                                          All Rights Reserved © 2012 IJARCET                                                      14
ISSN: 2278 – 1323
                                           International Journal of Advanced Research in Computer Engineering & Technology
                                                                                               Volume 1, Issue 2, April 2012


7.      Discussion and Conclusion
        In this paper on predator-prey system, a disease transmission model, incorporating
provisions for harvesting of prey have been discussed and analyzed. From the infected prey, the
disease is spreading to susceptible prey and consequently to the predator species. The predator-
prey species are compartmentalized into susceptible and infected classes. Recovery from disease
is not considered for both prey and the predator species. Consequently, SI model is considered
for both the species. SI model system admits four boundary equilibrium points and one non-zero
interior equilibrium point. The dynamic behavior of the system around each equilibrium point
has been studied and threshold values for basic reproduction numbers R0 and R1 are computed.

Conditions for the existence and stability of disease free prey predator system are obtained.
Conditions for endemic disease in prey species are discussed. Numerical Simulations are carried
out to confirm the results obtained analytically.
        It has been observed that the predator population becomes extinct and the disease dies out
from the prey population for sufficiently small feeding efficiency of predator when the basic
reproduction number R0 in prey population is below the threshold. If the basic reproduction

number R0 in the prey population is above the threshold, the disease in prey population
approaches endemic level and predator population becomes extinct. Disease in prey may be
responsible for elimination of predator.
        In case the feeding efficiency of predator population is sufficiently high so that
           rd 2
K1                 (r  e1 ) then the predator population persists.            When the basic reproduction
       (r  e1 )ka1

number R1 is below the threshold, then the disease dies out. The prey and predator population
                                                                             ˆ      ˆ
both go to their persistent equilibrium values and the equilibrium point E3 (S1 ,0, S2 ,0) is
stabilized. The difference in death rates of infected and susceptible species may be responsible
for instability of the equilibrium point E* (S1* , I1* , S2 , I 2 ) . Therefore, the disease may not be
                                                          *     *



endemic in prey predator system.
        It is observed that harvesting of infected prey helps in making the system disease free
where as harvesting of susceptible prey has adverse effect on it. Thus with an appropriate
                                                                                 ˆ      ˆ
harvesting of susceptible and infected prey, disease free equilibrium point E3 ( S1 ,0, S2 ,0) can be


                                   All Rights Reserved © 2012 IJARCET                                                   15
ISSN: 2278 – 1323
                                          International Journal of Advanced Research in Computer Engineering & Technology
                                                                                              Volume 1, Issue 2, April 2012


maintained at desired level. It is also observed that with harvesting of infected prey only, size of
prey and predator population is not affected where as removal of susceptible prey will not affect
the prey level but will reduce the predator level in disease free equilibrium state. Removal of both
susceptible and infected prey will make the system free from disease. At the same time it will
destabilize the predator free equilibrium point. If r  e1 , i.e if intrinsic growth rate of susceptible
prey is less than that of its harvesting from system then both the species will extinct from system.


       References:
                s
       [1]     A.P. Dobson, The population biology of parasite-induced changes in host
       behavior, Q. Rev. Biol. 63(1988), pp. 139-165.
       [2]     C. Castillo-Chavez, S. Blower, P. van der Driessche, D. Kirschner and A. A.
       Yakubu,      Mathematical Approaches for Emerging and Reemerging Infectious
       Diseases: An Introduction”, Journal of Theoretical Biology. Springer-Verlag, New
       York, 2002.
       [3]    E. Venturino, Epidemics in Predator-Prey Models: Disease in the Predators,
       IMA J. Math. Appl. Med. Biol. 19 (2002) 185-205.
       [4]    E. Venturino, On Epidemics Crossing the Species Barrier in Interacting
       Population Models, Varahmihir J. Math. Sci. 6 (2006) 247-263.
       [5]     E. Venturino, The influence of diseases on Lotka –Volterra system, Rky.
       Mt. J. Math. 24(1984), pp. 381-402.
       [6]     G. Birkhoff, G. C. Rota, Ordinary Differntial quations. Ginn Boston.(1982).
       [7]    H.W. Hethcote, Wendi Wang, L. Han, Z. Ma, A Predator-Prey Model With
       Infected Prey, Theor. Popul Biol. 66(2004) 259-268.
       [8]     J. Chattopadhyay, O. Arino, A predator-prey model with disease in the prey,
       Nonlinear Anal. 36(1999), pp. 747-766.
       [9]    J. Chattopadhyay, N. Bairagi, Pelicans at Risk in Salton Sea-An Eco-
       epidemiological Study, Ecol. Modell. 136 (2001) 103-112.
       [10]    J. Moore, Parasites and the Behavior of Animals, Oxford University
       Press,Oxford. 2002.
       [11] K.P. Hadeler, H.I. Freedman, Predator-Prey Populations With parasitic
       Infection, J. Math. Biol. 27(1989) 609-631.

                                   All Rights Reserved © 2012 IJARCET                                                  16
ISSN: 2278 – 1323
                                 International Journal of Advanced Research in Computer Engineering & Technology
                                                                                     Volume 1, Issue 2, April 2012


[12] L. Han, Z. Ma, H.W. Hethcote, Four Predator Prey Models With Infectious
Diseases, Math. Comput. Model. 34(2001) 849-858.
[13] N.     Nagumo,     Uber      die     lage       der      integeralkueven             gewonlicher
differentialgleichunger, Proc. Phys. Math. Soc. Japan, 24 (1942) 551.
[14]    O. Arino, A. El abdllaoui, J. Mikram, J. Chattopadhyay, Infection in Prey
Population May Act As Biological Control in Ratio-Dependent Predator-Prey
Models, Nonlinearity 17(2004) 1101-1116.
[15] O. Diekmann, J.A.P. Heesterbeek, J.A.J. Metz, On the Definition and the
Computation of the Basic Reproduction Ratio R0 in Models for Infectious Diseases
in Heterogeneous Populations, J. Math. Biol. 28(1990) 365-382.
[16]    P. van. der Driessche, J. Watmough, Reproduction Numbers and Sub-
threshold Endemic Equilibria for Compartmental Models of Disease Transmission,
Math. Biosci. 180(2002) 29-48.
[17]    R.M. Anderson and R.M. May, The invasion, persistence, and spread of
infectious diseases within animal and plant communities, Phillos. Trans. R. Soc.
Lond. B 314(1986), pp. 533-570.
[18]    R.M. Anderson, R.M. May, Regulation and Stability of Host-Parasite
Population Interactions I: Regulatory Processes, J. Anim. Ecol. 47(1978) 219-247.
[19] S. Gakkhar, K. B. Agnihotri, A Prey Predator System with Disease Crossing
Species Barrier, Proc. of International           Conference on Recent Advances in
Mathematical Sciences & Applications (RAMSA 2009), Vishakhapatnam, India, pp
296-303.
[20] S. Gakkhar, K. B. Agnihotri, S.I.S Model for Disease Transmission from
Prey to Predator, Journal of International Academy of Physical Sciences 14 (2010)
15-31
[21] S. Chaudhuri, A. Costamagna & E. Venturino, Epidemics spreading in
predator–prey systems, International Journal of Computer Mathematics, 89(2012)
561–584.




                         All Rights Reserved © 2012 IJARCET                                                   17

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  • 1. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 The dynamics of disease transmission in a Prey Predator System with harvesting of prey , Kul Bhushan Agnihotri* Department of Applied Sciences and Humanties Shaheed Bhagat Singh College of Engg & Tech Ferozepur-152004, Punjab, India Sunita Gakkhar ** Department of Mathematics, IIT Roorkee, Roorkee, India Abstract: In this present work on predator-prey system, a disease transmission model, incorporating provisions for harvesting of prey have been discussed and analyzed. The disease spread is from infected prey to predator species. The SI models are considered for both the species. Conditions are derived for existence and stability of disease free equilibrium state of the system. The effect of harvesting of prey has been analyzed from point view of the stability of system. The epidemiological threshold R0 and R1 quantities have been obtained using next generation approach for the model system. Conditions for endemic disease in prey species are discussed. This study also considers the impact of disease in prey on the extinction aspect of the predator. Numerical and computer simulations of the model have been done. Mathematics Subject Classification (2000) 35B35 - 92C05 - 92D30 -92D40 Keywords: Predator, prey, Equilibrium point, carrying capacity, Basic reproduction number, Stability, Harvesting 1. Introduction: Predator-prey interactions give regulatory system for the advancement of biological species. in natural ecosystem. Prey predator interactions and disease in the system affects each other [1, 3, 5, 7, 8-10, and 17]. Some previous studies of infectious diseases in animal populations were focused on the effects of disease-induced mortality or disease-reduced reproduction in the regulation of populations in their natural habitats [3, 7, 8, 17 and 18]. Reduced population sizes and destabilization of equilibrium into oscillations are caused by the presence of infectious disease in one or both of the populations. The fact that predators take a disproportionate number of infected preys has been confirmed by earlier studies [8, 11 and 17]. Infected prey is more exposed to predation on All Rights Reserved © 2012 IJARCET 1
  • 2. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 account of the fact that the disease may weaken their ability to protect themselves and expose them to predators [1]. This increased vulnerability of infected prey may lead to persistence of the predator (which would otherwise be starved and become extinct). Further, predation of the infected prey may lead to the disappearance of disease which may otherwise be endemic in prey population [3]. Together with no reproduction in infected prey, as predation on infected prey increases, the infection tends to destabilize prey-predator interactions [17]. Most of the eco-epidemiological studies are restricted to the situations where only prey species can get infection. Few investigations [4, 11, 19-21] consider the spread of disease from prey to predator through predation of infected prey. For the purpose of eliminating either the disease from predator- prey system or eliminating the menace of the predator by controlling disease in prey, a simplified eco- epidemiological four species prey predator SI model [4] is shown to be useful. Exploitation of biological resources as practiced in fishery, and forestry has strong impact on dynamic evolution of biological population. The over exploitation of resources may lead to extinction of species which adversely affects the ecosystem. However, reasonable and controlled harvesting is beneficial from economical and ecological point of view. The research on harvesting in predator-prey systems has been of interest to economists, ecologists and natural resource management for some time now. Very few has explicitly put a harvested parameter in a predator–prey–parasite model and studied its effect on the system. Here we study the role of harvesting in an eco-epidemiological system where the susceptible and infected prey are subjected to combined harvesting. In this present work on predator-prey system, a disease transmission model, incorporating provisions for harvesting of prey have been proposed and studied. In the model, the disease is spreading from infected prey to susceptible prey and consequently to the predator species via predation related activities: capturing, handling and eating the infected prey. Both, the prey and the predator species are compartmentalized into susceptible and infected classes. Recovery from disease is not considered for both prey and the predator species. Consequently, SI model is considered for both the species. 2. Mathematical Analysis Consider an eco-epidemiological system comprising of four populations, namely, the susceptible prey ( S1 ), infected prey ( I1 ), susceptible predator ( S 2 ) and infective predator ( I 2 ) All Rights Reserved © 2012 IJARCET 2
  • 3. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 such that N1  t   S1 (t )  I1 (t ) and N 2  t   S2 (t )  I 2 (t ) . An SI type eco-epidemiological model for prey predator dynamics is presented under following assumptions: Only susceptible prey is capable of reproducing logistically. While susceptible prey can easily escape the predation, the infected prey are weakened due to disease and become easier to catch. The infected prey and predator do not reproduce but still continue to consume resources. The susceptible predator gets food from infected prey for its survival. It may become infected due to interaction with infected prey. Mortality rate of infected predator is higher than that of susceptible predator. It is also assumed that the disease does not affect the hunting ability of infected predator. Further, all the predators who predate the infected prey become infected. Let e1 be the harvesting rate of susceptible prey and e2 be the harvesting rate of infected prey. Since it is easy to catch infected prey as compare to susceptible prey, therefore e1  e2 . Accordingly, the following mathematical model is obtained under the above assumptions: dS1  S I   rS1 1- 1 1  - a1S1 ( S2  I 2 ) - c1S1I1  e1S1 dt  K1  dI1  c1S1 I1 - a2 I1 ( S2  I 2 ) - d1 I1  e2 I1 dt dS2  -a2 S2 I1  (-d 2  ka1S1 ) S2 dt dI 2  a2 S2 I1 - d3 I 2 dt (1) where a1  Predation rate on the susceptible prey (hectare per individual day-1) a2  Predation rate on the infective prey (hectare per individual day-1) k  Feeding efficiency of predator (per individual day-1) r  Intrinsic growth rate constant of susceptible prey (day-1) K1  Carrying capacity of environment with respect to prey species (Individual ha-1) c1  Rate of force of infection (hectare per individual day-1) d1  Net death rate of prey (Natural death + death due to infection) (day-1) d 2  Natural death rate of susceptible predator (day-1) All Rights Reserved © 2012 IJARCET 3
  • 4. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 d3  Net death rate of infected predator (day ) -1 According to the assumptions a2  a1 , d3  d2 and e2  e1 , k  1. Also, S1 (0)  0, S2 (0)  0, I1 (0)  0 and I 2 (0)  0 . 3. Mathematical Analysis Theorem 1 All the solutions of the system (1) which initiate in  4 are uniformly bounded.  Proof: By theorems of Nagumo [13] , it can be easily proved that S1 , I1 , S 2 and I 2 remain positive. Let W1  S1  I1 From (1), the following can be easily obtained: d ( S1  I1 )  S   rS1 1- 1   e1S1 - d1I1  e2 I1 dt  K1  d (S1  I1 ) rS 2  (r  e1 )S1 - 1 - (d1  e2 ) I1 dt K1 For arbitrarily chosen 1 , this simplifies to d ( S1  I1 ) rS 2  1 ( S1  I1 )  (r  e1  1 ) S1 - 1 - (d1  e2  1 ) I1 dt K1 dW1 K1 (r  e1  1 ) 2 r  2 K1 K12 (r  e1  1 ) 2   1W1    S1  (r  e1  1 ) S1   - (d1  e2  1 ) I1 dt 4r K1  r 4r 2  K (r  e1  1 )2 r  2 dW1 K   1W1  1   S1  (r  e1  1 ) 1  - (d1  e2  1 ) I1 dt 4r K1  2r  Choosing 1  d1  e2 and applying the results of Birkhoff and Rota [6], yields L1 K1 (r  e1  1 )2 0  W1 ( S1 (t ), I1 (t ))  (1  e 1t )  W1 ( S1 (0), I1 (0))e 1t ; L1  1 4r As t   , it gives L1 0  S1  I1  ( K ) , 1  W1  S1  I1 is bounded From positivity of S1 and I1 , 0  S1  K ;0  I1  K . All Rights Reserved © 2012 IJARCET 4
  • 5. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 Similarly, defining another positive definite function W as W  S1  I1  S2  I 2 Proceeding in the similar manner and choosing   min(d1  e2 , d 2 , d3 ) yields L1 (r   ) 0  W ( S1 , I1 , S 2 .I 2 )  (1  e t )  W ( S1 (0), I1 (0), S 2 (0), I 2 (0))e t 1 As t   , it gives K (r   ) (r   ) 0 W   L , where L    W  S1  I1  S2  I 2 is bounded. 4 Hence all solutions of (1) that initiate in   are confined in the region  B  ( S1 , I1 , S2 , I 2 )   n : Si  L; I i  L; i  1, 2   4. Equilibrium points: The following equilibrium points exist for the system (1): a) The trivial equilibrium point E0 (0,0,0,0) b) The axial equilibrium point E1 ( S1 , 0, 0, 0) ,  K (r  e1 )  Where S1   1  always exist provided  r  r  e1 . (2) c) The planar equilibrium point E2 ( S1' , I1' ,0,0) in S1  I1 plane is obtained as d1  e2 ' c1K1 (r  e1 )  (d1  e2 )r S1'  , I1  , c1 c1 (c1K1  r ) The existence of this equilibrium point is possible provided c1K1 (r  e1 )  (d1  e2 )r  0 (3) In this case, the predator species is eliminated and the disease persists in the prey species. Harvesting of susceptible and infected prey will reduce the possibility of existence of All Rights Reserved © 2012 IJARCET 5
  • 6. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 E2 ( S1' , I1' ,0,0). If it exist then number of susceptible prey will increase but number of infected prey will decrease due to harvesting of susceptible and infected prey. ˆ ˆ Another disease free planar equilibrium point E3 (S1 ,0, S2 ,0) on S1  S2 plane exists provided ka1K1 (r  e1 )  rd2  0 (4) where ˆ d ˆ ka K (r  e )  rd 2 , S1  2 and, S2  1 1 2 1 ka1 ka1 K1 It has been also observed that even if the feeding efficiency k of predator is high enough d2 ˆ ˆ that K1  , even then the disease free equilibrium in E3 (S1 ,0, S2 ,0) may not exist with ka1 harvesting of susceptible prey. If it exists then number of susceptible prey will remain same but number of susceptible predator will decrease due to removal of susceptible prey. d) For non-zero equilibrium point E* (S1* , I1* , S1* , I1* ) of the system (1) is given by ˆ (r  e1 )a2 K1  a1c1K1S1'  (r  c1K1 )ka1S1 S1*  r (a2  ka1 )  a1c1K1 (1  k ) ˆ ka1 (S1*  S1 ) I1*  , S1*  I1*  K1 a2 c1d3 ( S1*  S1' ) S2  * , ˆ a2 (d3  (S1*  S1 )ka1 ) ˆ * ka1 ( S1*  S1 )S2 I2  * d3 Accordingly, E * (S * , I * , S * , I * ) exists provided S1*  max  S1' , S1   S , r  e1 ˆ (5) The Basic Reproduction Number is defined as the average number of secondary infections when one infective is introduced into a completely susceptible host population. It is also called the basic reproduction ratio or basic reproductive rate. Using next generation approach [2, 15 and 16], the epidemiological threshold quantities for the system (1) are obtained as All Rights Reserved © 2012 IJARCET 6
  • 7. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 c1K1 (r  e1 ) ˆ c1S1 R0  , R1  (6) r (d1  e2 ) ˆ d1  e2  a2 S2 Here, R0 is the basic reproduction number for isolated prey population and R1 is the basic reproduction in the prey population when both prey and predator are present in the system. The greater vulnerability of prey will reduce R1 . Harvesting of infected prey (e2 ) will reduce both R1 and R2 . Also by simplification it can be proved that R0  R1 5. Local Stability Analysis The variational matrix V of given system (1) is given by  2rS1 rI1 rS   r  K - a1 (S2  I 2 ) - c1I1 - K  e1 - 1 - c1S1 K1 -a1S1 -a1S1   1 1  V  c1I1 c1S1 - d1 - a2 (S2  I 2 )  e2 -a2 I1 -a2 I1     ka1S2 -a2 S2 -a2 I1  (-d 2  ka1S1 ) 0   -d 3   0 a2 S2 a2 I1  The following theorem is direct consequences of linear stability analysis of the system (1) about E0 and E1 . Theorem 2 The trivial equilibrium point E0 (0,0,0,0) is locally asymptotically stable provided r  e1 (7) Theorem 3 The axial equilibrium E1 ( S1 , 0, 0, 0) is locally asymptotically stable provided  ˆ S1  min S1' , S1  (8) The equilibrium E1 ( S1 , 0, 0, 0) is unstable when  S1  min  S1' , S1  ,  ˆ  (9) It can be concluded from (8) that E1 ( S1 , 0, 0, 0) may be stable for those parametric values for which it was not stable without harvesting of prey. So harvesting of susceptible and infected prey has positive effect on the stability of E1 ( S1 , 0, 0, 0). Also from (8) it may be noticed that when E1 ( S1 , 0, 0, 0) is locally asymptotically stable, All Rights Reserved © 2012 IJARCET 7
  • 8. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 d1  e2 d S1  and S1  2 , c1 ka1 (d1  e2 )r rd 2  K1  and K1  or c1 (r  e1 ) ka1 (r  e1 ) rd 2 R0  1 and K1  ka1 (r  e1 ) ˆ ˆ which violate existence conditions (3) and (4) of E2 ( S1' , I1' ,0,0) and E3 ( S1 ,0, S2 ,0) respectively. So, when E1 ( S1 , 0, 0, 0) is locally asymptotically stable then E0 (0,0,0,0), E2 ( S1' , I1' ,0,0) and ˆ ˆ E3 ( S1 ,0, S2 ,0) do not exist. When the perturbations are confined in S1  I1 plane only, then the equilibrium point E1 ( S1 , 0, 0, 0) is locally asymptotically stable for R0  1 . However in the presence of predator population the stability depends upon the dynamics of predator also as is evident from (8). In fact, when the feeding efficiency of predator is sufficiently low then the disease will die out from both the prey and predator under condition (8) and the equilibrium point E1 ( S1 , 0, 0, 0) is locally asymptotically stable. In other words, when the feeding efficiency is sufficiently low and the basic reproduction number R0 in prey population is below the threshold then predator population become extinct and disease dies out from the prey population. Theorem 4. If R0  1 , then E2 (S1' , I1' ,0,0) locally asymptotically stable provided ka1S1'  a2 I1'  d2  0 (10) Proof: From variational matrix V, the characteristic equation about E2 (S1' , I1' ,0,0) is obtained as  2 rS1'   rS '       c1 I1'  1  c1S1'   (a2 I1'  ka1S1'  d 2   ) (d3   )  0   K1  K1  The quadratic factor gives two eigen values with negative real parts . Therefore, the system around E2 (S1' , I1' ,0,0) is locally asymptotically stable provided (10) is satisfied.  If the basic reproduction number R0 in the prey population is above the threshold, the disease in prey population approaches to endemic level and predator population becomes extinct due to (10). All Rights Reserved © 2012 IJARCET 8
  • 9. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 Harvesting of susceptible and infected prey has negative effect on the stability of E2 (S1' , I1' ,0,0). The condition of instability of E2 (S1' , I1' ,0,0) if it exists, is given by ka1S1'  a2 I1'  d2  0 (11) ˆ ˆ Theorem 5. The disease free equilibrium state E3 ( S1 ,0, S2 ,0) , if it exists, is locally , asymptotically stable provided R1  1 . ˆ ˆ Proof: From variational matrix V, the characteristic equation about E3 ( S1 ,0, S2 ,0) is ˆ rS1 ( 2  ˆ ˆ ˆ ˆ   ka12 S1S2 )(c1S1  a2 S2  d1  e2   )(d3   )  0 K1 Since the quadratic factor always yield eigen values with negative real parts, the condition for stability is ˆ ˆ c1S1  a2 S2  d1  e2  0 Its simplification gives R1  1 (12) This completes the proof.  When the basic reproduction number R1 is below the threshold, then the disease dies out ˆ ˆ from both the species and the equilibrium point E3 ( S1 ,0, S2 ,0) is stabilized. Rewriting stability condition gives the critical value of e2 for which the disease free equilibrium state is locally asymptotically stable:  ra  ˆ a ˆ d e2   c1  2  S1  2 (r  e1 )  d1 , S1  2  K1a1  a1 ka1 (13) The greater vulnerability of prey to predation may be responsible for persistence of disease free prey predator population. By simplifying above condition for stability it has been observed that harvesting of ˆ ˆ infected prey may improve the stability of equilibrium point E3 ( S1 ,0, S2 ,0) where as it become less stable with harvesting of susceptible prey. Thus with an appropriate harvesting of ˆ ˆ susceptible and infected prey, disease free equilibrium point E3 ( S1 ,0, S2 ,0) can be maintained at desired level. All Rights Reserved © 2012 IJARCET 9
  • 10. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 ˆ ˆ The disease free equilibrium state E3 ( S1 ,0, S2 ,0) if it exist, is unstable if ˆ ˆ c1S1  a2 S2  d1  e2  0 (14) It is observed that E2 (S1' , I1' ,0,0) , if it exists, is locally asymptotically stable provided ˆ ˆ E3 ( S1 ,0, S2 ,0) is unstable and vice-versa. However, it is possible for some choice of parameters that both E2 ( S1, I1, 0, 0) and ˆ ˆ E3 (S1 ,0, S2 ,0) exist and locally stable. ˆ ˆ It is also observed that when both E2 ( S1, I1, 0, 0) and E3 (S1 ,0, S2 ,0) are stable then non-zero equilibrium point E* (S1* , I1* , S2* , I 2* ) always exist. Theorem 6. The non-zero equilibrium point E* (S1* , I1* , S1* , I1* ) , if exists, is a saddle point. Proof: The characteristic equation about E* is obtained as  4  A0 3  A1 2  A2  A3  0 (15) Where  r  A3  a2 (d3  a2 I1* ) (k  1)a1c1   ka1  a2   I1*S1*S 2 *  K1  As the constant term A3 is always negative, at least one eigenvalue of the equation (15) will be positive, therefore E* (S1* , I1* , S2 , I 2 ) is not locally asymptotically stable. * * It is either unstable or a saddle point. □ 6. Numerical simulations Numerical simulations have been carried out to investigate dynamics of the proposed model. Computer simulations have been performed on MATLAB for different set of parameters. Consider the following set of parametric values: r  0.1, K1  50, e1  0.03, e2  0.05, d1  0.7, d 2  0.6, (16) d3  0.7, c1  0.01, a1  0.8, a2  0.9, k  0.012 The system (1) has equilibrium point E1 (35, 0, 0, 0) for the data set (16). It is locally asymptotically stable by the computed value of R0 is 0.4667  1 and the value of feeding efficiency k of predator population is sufficiently low and the condition (8) is satisfied. The solution trajectories in phase space S1  I1  S2 are drawn in Fig. 1 for different initial values. All All Rights Reserved © 2012 IJARCET 10
  • 11. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 the solution trajectories to tend to E1 (35, 0, 0, 0). D 20 15 A=( 1, 10, 10, 1 ) 10 B=( 20, 0, 10, 0 ) S2 A C=( 20, 10, 0, 0 ) 5 B D=( 20, 20, 20, 20 ) 0 20 C E1 E =( 35, 0, 0, 0 ) 1 15 10 30 5 20 10 I1 0 0 S1 Fig 1: Phase plot depicting the stability of equilibrium point E1 in phase space S1 - I1 - S2 for data-set (16) Now consider following set of data r  0.02, K1  100, e1  0.021, e2  0.03, d1  0.01, d 2  0.11, (17) d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33 For above set of data, the equilibrium point E0 (0, 0, 0, 0) is locally asymptotically stable as r  e1 (see Fig. 2) and all other equilibrium points do not exist. 20 D 15 A=( 1, 10, 10, 1 ) 10 S2 B=( 20, 0, 10, 0 ) 5 A C=( 20, 10, 0, 0 ) 0 B D=( 20, 20, 20, 20 ) 20 C 15 E0=( 0, 0, 0, 0 ) 10 5 30 20 I1 0 10 0 E0 S1 All Rights Reserved © 2012 IJARCET 11
  • 12. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 Fig 2: Phase plot depicting the stability of equilibrium point E1 in phase space S1 - I1 - S2 for data set 17 For the following data set of parameters, E2 is stable and E3 is unstable: r  0.02, K1  100, e1  0.01, e2  0.03, d1  0.01, d 2  0.11, (18) d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33 The equilibrium point E1 (50, 0, 0, 0) is unstable as condition (8) is not satisfied and both the planar equilibrium points E2 (20, 2.7273, 0, 0) and E3 (33.3333, 0, 0.3333, 0) exists condition (3) and (4) are satisfied respectively. The equilibrium point E3 (33.3333, 0, 0.3333, 0) is found to be unstable as it satisfies the condition (14). The equilibrium point E2 (20, 2.7273, 0, 0) is found to be locally asymptotically stable as condition (10) is satisfied. The solution trajectories in phase space S1  I1  S2 are drawn in Fig. 4 for different initial values. All these trajectories converge to E2 (20, 2.7273, 0, 0) . Starting with initial value in the neighborhood of the point E3 (33.3333, 0, 0.3333, 0) , the solution trajectory approaches to the equilibrium point E2 (20, 2.7273, 0, 0). This confirms the instability of E3 . 20 D E2=(20, 2.7273, 0, 0) 15 A=(0.1, 0.1, 0.1,0.1) 10 S2 5 B=(50, 0.1, 0.1, 0.1) 0 C=(33.33,0.1,0.33,0.1) 20 15 E2 B D=(20, 20, 20, 20) C 10 50 A 40 5 30 20 I1 0 10 0 S1 Fig. 3: Phase plot depicting the stability of E2 and instability of E3 in S1  I1  S 2 space for dataset (18) All Rights Reserved © 2012 IJARCET 12
  • 13. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 The following data is selected for which all the equilibrium points exist: r  0.02, K1  100, e1  0.01, e2  0.068, d1  0.01, d 2  0.11, (19) d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33 In this case, the equilibrium point E1 (50, 0, 0, 0) is unstable. It is observed that both the equilibrium points E2 (39, 1, 0, 0) and E3 (33.3333, 0, 0.3333, 0) are locally asymptotically stable. The point E2 (39, 1, 0, 0) is stable since ka1S1'  d3 I1'  d2  0.0013  0 and R0  1.2821  1 . Also, E3 (33.3333, 0, 0.3333, 0) is locally asymptotically stable as R1  0.7874  1 . Both the equilibrium points have their own domains of attractions. Trajectories with different initial conditions converge to different equilibrium points (See Fig. 4). The instability of non-zero equilibrium point E* (39.0915,0.9501,0.0081,0.0010) can be seen from Fig. 4. It is also noticed that when even a very small perturbation is taken from E* (39.0915,0.9501,0.0081,0.0010) to D(40, 0.9501, 0.0081, 0.0010) , along S1 direction, the trajectory converges to E2 (39, 1, 0, 0) . Whereas, when the perturbation is taken to E (39.0915,1, 0.0081, 0.0010) , the trajectory of the system converges to E3 (33.3333, 0, 0.3333, 0) . A=(0.1, 0.1, 0.1,0.1) B=(50, 0.1, 0.1, 0.1) C=(1, 1, 1, 1) D=(40, 0.9501, 0.0081, 0.0010) E=(39.0915, 1, 0.0081,0.00100) E2=(39,1, 0, 0) 1 E3=(33.3333,0.3333,0,0) E3 A S2 0.5 C 0 0 B 0.5 D 0 I1 E 10 E 2 20 1 30 40 50 S1 Fig 4: Phase plot depicting the stable behaviour of E2 , E3 in S1  I1  S2 space for dataset (19) All Rights Reserved © 2012 IJARCET 13
  • 14. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 Now, consider the following data set where E3 is stable and E2 unstable: r  0.02, K1  100, e1  0.01, e2  0.069, d1  0.01, d 2  0.11, (20) d3  0.15, c1  0.002, a1  0.01, a2  0.02, k  0.33 d2 (d1  e2 ) As S1 ( 50) is greater than computed value 33.3333 of and 39.5 of in this case, ka1 c1 the equilibrium point E1 (50, 0, 0, 0) is unstable and system (1) has two planar equilibrium points, say E2 (39.5, 0.9545, 0, 0) and E3 (33.3333, 0, 0.3333, 0) . The equilibrium point E3 (33.3333, 0, 0.3333, 0) is found to be stable as it satisfies the condition (12). The equilibrium point E2 (39.5, 0.9545, 0, 0) is found to be unstable as it satisfies the condition (11). The solution trajectories in phase space S1 - I1 - S2 are drawn in Fig. 5 for different initial values. All these trajectories approach to E3 (33.3333, 0, 0.3333, 0) . Convergence of solution trajectory to equilibrium E3 (33.3333, 0, 0.3333, 0) with initial value near E2 (39.5, 0.9545, 0, 0) also confirms the instability of E2 (39.5, 0.9545, 0, 0) . A=(0.1, 0.1, 0.1,0.1) B=(50, 0.1, 0.1, 0.1) C=(1, 1, 1, 1) D=(39.5, 0.9545, 0.1, 0.1) E3=(33.3333, 0, 0.3333,0) 1.5 1 C S2 E3 0.5 A B 0 0 D 10 0 0.5 20 30 1 40 I1 50 S1 Fig. 5: Phase plot depicting the stability of E3 and instability of E2 in S1  I1  S 2 space for dataset (20) All Rights Reserved © 2012 IJARCET 14
  • 15. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 7. Discussion and Conclusion In this paper on predator-prey system, a disease transmission model, incorporating provisions for harvesting of prey have been discussed and analyzed. From the infected prey, the disease is spreading to susceptible prey and consequently to the predator species. The predator- prey species are compartmentalized into susceptible and infected classes. Recovery from disease is not considered for both prey and the predator species. Consequently, SI model is considered for both the species. SI model system admits four boundary equilibrium points and one non-zero interior equilibrium point. The dynamic behavior of the system around each equilibrium point has been studied and threshold values for basic reproduction numbers R0 and R1 are computed. Conditions for the existence and stability of disease free prey predator system are obtained. Conditions for endemic disease in prey species are discussed. Numerical Simulations are carried out to confirm the results obtained analytically. It has been observed that the predator population becomes extinct and the disease dies out from the prey population for sufficiently small feeding efficiency of predator when the basic reproduction number R0 in prey population is below the threshold. If the basic reproduction number R0 in the prey population is above the threshold, the disease in prey population approaches endemic level and predator population becomes extinct. Disease in prey may be responsible for elimination of predator. In case the feeding efficiency of predator population is sufficiently high so that rd 2 K1  (r  e1 ) then the predator population persists. When the basic reproduction (r  e1 )ka1 number R1 is below the threshold, then the disease dies out. The prey and predator population ˆ ˆ both go to their persistent equilibrium values and the equilibrium point E3 (S1 ,0, S2 ,0) is stabilized. The difference in death rates of infected and susceptible species may be responsible for instability of the equilibrium point E* (S1* , I1* , S2 , I 2 ) . Therefore, the disease may not be * * endemic in prey predator system. It is observed that harvesting of infected prey helps in making the system disease free where as harvesting of susceptible prey has adverse effect on it. Thus with an appropriate ˆ ˆ harvesting of susceptible and infected prey, disease free equilibrium point E3 ( S1 ,0, S2 ,0) can be All Rights Reserved © 2012 IJARCET 15
  • 16. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 maintained at desired level. It is also observed that with harvesting of infected prey only, size of prey and predator population is not affected where as removal of susceptible prey will not affect the prey level but will reduce the predator level in disease free equilibrium state. Removal of both susceptible and infected prey will make the system free from disease. At the same time it will destabilize the predator free equilibrium point. If r  e1 , i.e if intrinsic growth rate of susceptible prey is less than that of its harvesting from system then both the species will extinct from system. References: s [1] A.P. Dobson, The population biology of parasite-induced changes in host behavior, Q. Rev. Biol. 63(1988), pp. 139-165. [2] C. Castillo-Chavez, S. Blower, P. van der Driessche, D. Kirschner and A. A. Yakubu, Mathematical Approaches for Emerging and Reemerging Infectious Diseases: An Introduction”, Journal of Theoretical Biology. Springer-Verlag, New York, 2002. [3] E. Venturino, Epidemics in Predator-Prey Models: Disease in the Predators, IMA J. Math. Appl. Med. Biol. 19 (2002) 185-205. [4] E. Venturino, On Epidemics Crossing the Species Barrier in Interacting Population Models, Varahmihir J. Math. Sci. 6 (2006) 247-263. [5] E. Venturino, The influence of diseases on Lotka –Volterra system, Rky. Mt. J. Math. 24(1984), pp. 381-402. [6] G. Birkhoff, G. C. Rota, Ordinary Differntial quations. Ginn Boston.(1982). [7] H.W. Hethcote, Wendi Wang, L. Han, Z. Ma, A Predator-Prey Model With Infected Prey, Theor. Popul Biol. 66(2004) 259-268. [8] J. Chattopadhyay, O. Arino, A predator-prey model with disease in the prey, Nonlinear Anal. 36(1999), pp. 747-766. [9] J. Chattopadhyay, N. Bairagi, Pelicans at Risk in Salton Sea-An Eco- epidemiological Study, Ecol. Modell. 136 (2001) 103-112. [10] J. Moore, Parasites and the Behavior of Animals, Oxford University Press,Oxford. 2002. [11] K.P. Hadeler, H.I. Freedman, Predator-Prey Populations With parasitic Infection, J. Math. Biol. 27(1989) 609-631. All Rights Reserved © 2012 IJARCET 16
  • 17. ISSN: 2278 – 1323 International Journal of Advanced Research in Computer Engineering & Technology Volume 1, Issue 2, April 2012 [12] L. Han, Z. Ma, H.W. Hethcote, Four Predator Prey Models With Infectious Diseases, Math. Comput. Model. 34(2001) 849-858. [13] N. Nagumo, Uber die lage der integeralkueven gewonlicher differentialgleichunger, Proc. Phys. Math. Soc. Japan, 24 (1942) 551. [14] O. Arino, A. El abdllaoui, J. Mikram, J. Chattopadhyay, Infection in Prey Population May Act As Biological Control in Ratio-Dependent Predator-Prey Models, Nonlinearity 17(2004) 1101-1116. [15] O. Diekmann, J.A.P. Heesterbeek, J.A.J. Metz, On the Definition and the Computation of the Basic Reproduction Ratio R0 in Models for Infectious Diseases in Heterogeneous Populations, J. Math. Biol. 28(1990) 365-382. [16] P. van. der Driessche, J. Watmough, Reproduction Numbers and Sub- threshold Endemic Equilibria for Compartmental Models of Disease Transmission, Math. Biosci. 180(2002) 29-48. [17] R.M. Anderson and R.M. May, The invasion, persistence, and spread of infectious diseases within animal and plant communities, Phillos. Trans. R. Soc. Lond. B 314(1986), pp. 533-570. [18] R.M. Anderson, R.M. May, Regulation and Stability of Host-Parasite Population Interactions I: Regulatory Processes, J. Anim. Ecol. 47(1978) 219-247. [19] S. Gakkhar, K. B. Agnihotri, A Prey Predator System with Disease Crossing Species Barrier, Proc. of International Conference on Recent Advances in Mathematical Sciences & Applications (RAMSA 2009), Vishakhapatnam, India, pp 296-303. [20] S. Gakkhar, K. B. Agnihotri, S.I.S Model for Disease Transmission from Prey to Predator, Journal of International Academy of Physical Sciences 14 (2010) 15-31 [21] S. Chaudhuri, A. Costamagna & E. Venturino, Epidemics spreading in predator–prey systems, International Journal of Computer Mathematics, 89(2012) 561–584. All Rights Reserved © 2012 IJARCET 17