International Journal of Bioinformatics and Biomedical Engineering, Vol. 1, No. 2, September 2015 Publish Date: Aug. 24, 2015 Pages: 153-161

A Study on Discrete Model of Three Species Syn Eco System with Unlimited Resources for the Second Species

B. Hari Prasad*

Department of Mathematics, Chaitanya Degree College (Autonomous), Hanamkonda, Telangana State, India

Abstract

In this paper, the three species syn eco-system comprises of a commensal (S1), two hosts S2 and S3 ie., S2 and S3 both benefit S1, without getting themselves effected either positively or adversely. Further S2 is a commensal of S3, S3 is a host of both S1, S2 and the second species has unlimited resources. The basic equations for this model constitute as three first order non-linear coupled ordinary difference equations. All possible equilibrium points are identified based on the model equations at two stages and criteria for their stability are discussed. Further the numerical solutions are computed for specific values of the various parameters and the initial conditions.

Keywords

Commensal, Equilibrium Point, Host, Oscillatory, Stable, Unstable


1. Introduction

Ecology, a branch evolutionary biology, deals with living species that coexist in a physical environment sustain themselves on common resources. It is a common observations that the species of same nature can not flourish is isolation without any interaction with species of different kinds. Significant researches in the area of theoretical ecology have been discussed by Kot [1] and by [2]. Several ecologists and mathematicians contributed to the growth of this area of knowledge. Mathematical ecology can be broadly divided into two main sub-divisions, Autecology and Synecology, which are described in the treatises of Arumugam [3], Sharma [4]. Syn-ecology is an ecosystem comprised of two or more distinct species. Species interact with each other in one way or other. The Ecological interactions can be classified as Ammensalism, Competition, Commensalism, Neutralism, Mutualism, Predation, Parasitism and so on.

Mathematical Modeling plays a vital role in providing insight into the mutual relationships (positive, negative) between the interacting species. The general concepts of Modeling in Biological Science have been initiated by several authors Ma [5], Murray [6], and Sze-Bi Hsu [7]. Recently the authors Papa Rao et al. [8], Shivareddy et al. [9], Srinivas [10] and Kumar et al. [11] discussed three species ecological models such as predation, completion and commensalism. Srinivas [12] studied the competitive ecosystem of two species and three species with limited and unlimited resources. Later, Narayan et al. [13] studied prey-predator ecological models with partial cover for the prey and alternate food for the predator. Acharyulu et al. [14,15] derived some productive results on various mathematical models of ecological Ammensalism with multifarious resources in the manifold directions. Further, Kumar [16] studied some mathematical models of ecological commensalism. The present author Prasad [17-22] investigated continuous and discrete models on the three species syn-ecosystems.

The present investigation is on an analytical study of a typical three species (S1, S2, S3) syn-eco system. The system comprises of a commensal (S1), two hosts S2 and S3 ie, S2 and S3 both benefit S1, without getting themselves effected either positively or adversely. Further S2 is a commensal of S3 and S3 is a host of both S1, S2. Commensalism is a symbiotic interaction between two populations where one population (S1) gets benefit from (S2) while the other (S2) is neither harmed nor benefited due to the interaction with (S1). The benefited species (S1) is called the commensal and the other, the helping one (S2) is called the host species. A common example is an animal using a tree for shelter-tree (host) does not get any benefit from the animal (commensal). Some more real-life examples of commensalism are, i. The clownfish shelters among the tentacles of the sea anemone, while the sea anemone is not affected. ii. A flatworm attached to the horse crab and eating the crab’s food, while the crab is not put to any disadvantage. iii. Sucker fish (echeneis) gets attached to the under surface of sharks by its sucker. This provides easy transport for new feeding grounds and also food pieces falling from the sharks prey, to Echeneis.

2. Basic Equations of the Model

2.1. Notation Adopted

Ni(t) : The population strength of Si at time t, i = 1,2,3; t: Time instant ; ai: Natural growth rate of Si , i = 1, 2, 3; aii: Self inhibition coefficients of Si, i = 1, 3; a12, a13: Interaction coefficients of S1 due to S2 and S1 due to S3; a23 : Interaction coefficient of S2 due to S3. Further the variables N1, N2, N3 are non-negative and the model parameters a1, a2, a3, a11, a12, a33, a13, a23 are assumed to be non-negative constants.

2.2. Basic Equations

Consider the growth of the species during the time interval.

     (1)

           (2)

                (3)

The equations (1), (2) and (3) can be written in the nonlinear autonomous system of discrete equations as

      (4)

                   (5)

                       (6)

where .

3. Equilibrium States

The equilibrium states for a discrete model are defined in terms of the period of no growth. i.e,   where r is the period of the equilibrium state.

3.1. One Period Equilibrium States

.

The system under investigation has five equilibrium states given by

3.2. The Stability Analysis of One Period Equilibrium States

3.2.1. The Stability of E1

, where r is an integer and i = 1, 2, 3.

Hence, E1 (0, 0, 0) is stable.

3.2.2. The Stability of E2

where r is an integer and i = 1, 2.

Hence, E2 is stable.

3.2.3. The Stability of E3

where r is an integer and i = 2, 3.

Hence, E3 is stable.

3.2.4. The Stability of E4

Hence, E4 is stable.

3.2.5. The Stability of E5

where r is an integer.

Hence, E5 is stable.

At this stage all the five equilibrium states are stable.

3.3. Two Period Equilibrium States

The system under investigation has twenty five equilibrium states given by

.

The states E3 and E4 coincide when α3 = 3 and do not exist when α3 < 3.

.

The states E7and E8 coincide when α1 = 3 and do not exist when α1 < 3.

The states E11and E12 coincide when β1 = 3 and do not exist when β1 < 3.

The states E15 and E16 coincide when γ1 = 3 and do not exist when γ 1 < 3.

The states E19 and E20 coincide when µ1 = 3 and do not exist when µ1 < 3.

The states E23 and E24 coincide when δ1 = 3 and do not exist when δ 1 < 3.

3.4. The Stability Analysis of Two Period Equilibrium States

The equilibrium states E1, E2 and E6 are stable as established in 3.2. Now we will discuss the stability of other equilibrium states except these three states.

3.4.1. The Stability of E3

, where r is an integer and i = 1, 2.

where r is an integer.

Hence, E3 oscillates between

,

when α3 > 3and is stable when α3 = 3.

3.4.2. The Stability of E4

, where r is an integer and i = 1, 2.

where r is an integer.

Hence, E4 oscillates between

,

when α3 > 3and is stable when α3 = 3.

3.4.3. The Stability of E5

where r is an integer and i = 1, 2.

Hence, E5 is stable.

3.4.4. The Stability of E7

where r is an integer.

, where r is an integer and i = 2, 3.

Hence, E7 oscillates between

,

when α1 > 3and is stable when α1 = 3.

3.4.5. The Stability of E8

where r is an integer.

, where r is an integer and i = 2, 3.

Hence, E8 oscillates between

,

when α1 > 3and is stable when α1 = 3.

3.4.6. The Stability of E9

where r is an integer and i = 2, 3.

Hence, E9 is stable.

3.4.7. The Stability of E10

where  is an integer.

Hence, E10 is stable.

3.4.8. The Stability of E11

 where r is an integer.

Hence, E11 oscillates between

,

when β1 > 3and is stable when β1 = 3.

3.4.9. The Stability of E12

 where r is an integer.

Hence, E12 oscillates between

,

when β1 > 3and is stable when β1 = 3.

3.4.10. The Stability of E13

 

where r is an integer.

Hence, E13 is stable.

3.4.11. The Stability of E14

 where  is an integer except 0 and 1

 

where  is an integer.

Hence, E14 is unstable, when α3 > 3and is stable when α3 = 3.

3.4.12. The Stability of E15

where  is an integer except 0 and 1

 

where  is an integer.

Hence, E15 is unstable, when α3 > 3and is oscillatory when α3 = 3.

3.4.13. The Stability of E16

 

where  is an integer except 0 and 1.

 

where  is an integer.

Hence, E16 is unstable, when α3 > 3and is oscillatory when  α3 = 3.

3.4.14. The Stability of E17

 where  is an integer except 0 and 1

 

where  is an integer.

Hence, E17 is unstable, when α3 > 3and is stable when α3 = 3.

3.4.15. The Stability of E18

 where  is an integer except 0 and 1.

 

where  is an integer.

Hence, E14 is unstable, when α3 > 3and is stable when α3 = 3.

3.4.16. The Stability of E19

where  is an integer except 0 and 1.

where  is an integer.

Hence, E19 is unstable, when α3 > 3and is oscillatory when  α3 = 3.

3.4.17. The Stability of E20

 

where  is an integer except 0 and 1.

 

where  is an integer.

Hence, E20 is unstable, when α3 > 3and is oscillatory when  α3 = 3.

3.4.18. The Stability of E21

 where  is an integer except 0 and 1.

 

where  is an integer.

Hence, E21 is unstable, when α3 > 3and is stable when α3 = 3.

3.4.19. The Stability of E22

where  is an integer.

Hence, E22 is stable.

3.4.20. The Stability of E23

where r is an integer.

Hence, E23 oscillates between

,

when δ1 > 3and is stable when δ1 = 3.

3.4.21. The Stability of E24

where r is an integer.

Hence, E24 oscillates between

,

when δ1 > 3and is stable when δ1 = 3.

3.4.22. The Stability of E25

where  is an integer.

Hence, E25 is stable, when δ3 = 3and α3 = 3.

At this stage, in all twenty five equilibrium states, only the nine states E1, E2, E5, E6, E9,E10, E13, E22, E25 are stable and E3, E4, E7, E8, E11, E12, E23, E24 are oscillatory and remaining all are unstable.

4. Numerical Examples

Figure 1. Variation of population against time for a1 = 1.5, a11 = 1, a13 = 0.4, a2 = 1.05, a22 = 3.4, a23 = 4.53, a3 = 2.7, a33 = 0.3, N1(0) = 6.1, N2(0) = 0, N3(0) = 9.

Figure 2. Variation of population against time for a1 = 3.6, a11 = 0.3, a13 = 2.6, a2 = 4.7, a22 = 1.28, a23 = 3.33, a3 = 1.23, a33 = 2.1, N1(0) = 14.32, N2(0) = 0, N3(0) = 0.

The numerical solutions of the discrete model equations computed for specific values of the various parameters and the initial conditions. The results are illustrated in Figures 1 to 4.

Figure 3. Variation of population against time for a1 = 1.5, a11 = 1.2, a13 = 0.4, a2 = 2.11, a22 = 1.4, a23 = 0.50, a3 = 1.6, a33 = 0.2, N1(0) = 8.6, N2(0) = 0, N3(0) = 8.

Figure 4. Variation of population against time for a1 = 2.6, a11 = 1.29, a13 = 0.01, a2 = 0.7, a22 = 1.53, a23 = 0.85, a3 = 3.6, a33 = 0.3, N1(0) = 2.1, N2(0) = 0, N3(0) = 14.32.

5. Discussion and Conclusions

The present paper deals with an investigation on a discrete model of three species syn eco-system with unlimited resources for the second species. The system comprises of a commensal (S1) common to two hosts S2 and S3 ie., S2 and S3 both benefit S1, without getting themselves effected either positively or adversely. Further S2 is a commensal of S3, S3 is a host of both S1, S2. All possible equilibrium points of the model are identified based on the model equations at two stages.

Stage-I: Ni (t + 1) = Ni (t); i = 1, 2, 3.

Stage-II: Ni (t + 2) = Ni (t); i = 1, 2, 3.

In Stage-I there are only five equilibrium points, while the Stage-II there would be twenty five equilibrium points. All the five equilibrium points in Stage-I are found to be stable while in stage-II only nine are stable. Further the numerical solutions for the discrete model equations are computed.

Acknowledgment

I thank to Professor (Retd), N.Ch. Pattabhi Ramacharyulu, Department of Mathematics, National Institute of Technology, Warangal (T.S.), India for his valuable suggestions and encouragement.

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