A Mathematical study of Two Species Amensalism Model With a Cover for the first Species by Homotopy Analysis Method

Similar documents
Application of Homotopy Analysis Method for Solving various types of Problems of Partial Differential Equations

On Control Problem Described by Infinite System of First-Order Differential Equations

Stress Analysis of Infinite Plate with Elliptical Hole

Lecture 18: Kinetics of Phase Growth in a Two-component System: general kinetics analysis based on the dilute-solution approximation

STUDY OF THE STRESS-STRENGTH RELIABILITY AMONG THE PARAMETERS OF GENERALIZED INVERSE WEIBULL DISTRIBUTION

7 Wave Equation in Higher Dimensions

Lecture-V Stochastic Processes and the Basic Term-Structure Equation 1 Stochastic Processes Any variable whose value changes over time in an uncertain

International Journal of Pure and Applied Sciences and Technology

HAM for finding solutions to coupled system of variable coefficient equations arising in fluid dynamics

Sections 3.1 and 3.4 Exponential Functions (Growth and Decay)

TIME DELAY BASEDUNKNOWN INPUT OBSERVER DESIGN FOR NETWORK CONTROL SYSTEM

Synchronization of Fractional Chaotic Systems via Fractional-Order Adaptive Controller

ÖRNEK 1: THE LINEAR IMPULSE-MOMENTUM RELATION Calculate the linear momentum of a particle of mass m=10 kg which has a. kg m s

An approximate solution for a generalized Hirota-Satsom coupled (Kdv) equation

AN EVOLUTIONARY APPROACH FOR SOLVING DIFFERENTIAL EQUATIONS

On The Estimation of Two Missing Values in Randomized Complete Block Designs

Fig. 1S. The antenna construction: (a) main geometrical parameters, (b) the wire support pillar and (c) the console link between wire and coaxial

An Automatic Door Sensor Using Image Processing

Analytical Solution for the Time-Dependent Emden-Fowler Type of Equations by Homotopy Analysis Method with Genetic Algorithm

336 ERIDANI kfk Lp = sup jf(y) ; f () jj j p p whee he supemum is aken ove all open balls = (a ) inr n, jj is he Lebesgue measue of in R n, () =(), f

Lecture 17: Kinetics of Phase Growth in a Two-component System:

THE FINITE HAUSDORFF AND FRACTAL DIMENSIONS OF THE GLOBAL ATTRACTOR FOR A CLASS KIRCHHOFF-TYPE EQUATIONS

On the Semi-Discrete Davey-Stewartson System with Self-Consistent Sources

MEEN 617 Handout #11 MODAL ANALYSIS OF MDOF Systems with VISCOUS DAMPING

Optimum Settings of Process Mean, Economic Order Quantity, and Commission Fee

BMOA estimates and radial growth of B φ functions

General Non-Arbitrage Model. I. Partial Differential Equation for Pricing A. Traded Underlying Security

EFFECT OF PERMISSIBLE DELAY ON TWO-WAREHOUSE INVENTORY MODEL FOR DETERIORATING ITEMS WITH SHORTAGES

ON 3-DIMENSIONAL CONTACT METRIC MANIFOLDS

4. Fundamental of A.C. Circuit

Robust Output Command Tracking for Linear Systems with Nonlinear Uncertain Structure with Application to Flight Control

A Prey-Predator Model with an Alternative Food for the Predator and Optimal Harvesting of the Prey

Research Article A Note on Multiplication and Composition Operators in Lorentz Spaces

KINEMATICS OF RIGID BODIES


Combinatorial Approach to M/M/1 Queues. Using Hypergeometric Functions

Research Article Strategic Conditions for Opening an Internet Store and Pricing Policies in a Retailer-Dominant Supply Chain

Exponential and Logarithmic Equations and Properties of Logarithms. Properties. Properties. log. Exponential. Logarithmic.

Adsorption and Desorption Kinetics for Diffusion Controlled Systems with a Strongly Concentration Dependent Diffusivity

Trajectory estimation based on extended state observer with Fal-filter

An Analytical Study of Strong Non Planer Shock. Waves in Magnetogasdynamics

Chapter 2. First Order Scalar Equations

Solution of Integro-Differential Equations by Using ELzaki Transform

The Global Trade and Environment Model: GTEM

VOL. 1, NO. 8, November 2011 ISSN ARPN Journal of Systems and Software AJSS Journal. All rights reserved

r r r r r EE334 Electromagnetic Theory I Todd Kaiser

Method for simulation of the fractional order chaotic systems

Introduction to Numerical Analysis. In this lesson you will be taken through a pair of techniques that will be used to solve the equations of.

The sudden release of a large amount of energy E into a background fluid of density

MATHEMATICAL FOUNDATIONS FOR APPROXIMATING PARTICLE BEHAVIOUR AT RADIUS OF THE PLANCK LENGTH

Exact solitary-wave Special Solutions for the Nonlinear Dispersive K(m,n) Equations by Means of the Homotopy Analysis Method

Analytical solution for nonlinear Gas Dynamic equation by Homotopy Analysis Method

DYNAMIC ION BEHAVIOR IN PLASMA SOURCE ION IMPLANTATION BİLGE BOZKURT

Lecture 5. Chapter 3. Electromagnetic Theory, Photons, and Light

Dynamics in a discrete fractional order Lorenz system

Research on the Algorithm of Evaluating and Analyzing Stationary Operational Availability Based on Mission Requirement

Orthotropic Materials

Oscillation Properties of a Logistic Equation with Several Delays

An Exact Solution of Navier Stokes Equation

b denotes trend at time point t and it is sum of two

Homotopy Perturbation Method for Solving Some Initial Boundary Value Problems with Non Local Conditions

Lecture 22 Electromagnetic Waves

Variance and Covariance Processes

Chapter 5. Canopy Spectral Invariants

Heat Conduction Problem in a Thick Circular Plate and its Thermal Stresses due to Ramp Type Heating

Section 3.5 Nonhomogeneous Equations; Method of Undetermined Coefficients

Analytical Solutions of an Economic Model by the Homotopy Analysis Method

Two-Pion Exchange Currents in Photodisintegration of the Deuteron

An assessment of ring seine fishery in Kerala through surplus production model

arxiv: v1 [math.gm] 4 Nov 2018

POSITIVE SOLUTIONS WITH SPECIFIC ASYMPTOTIC BEHAVIOR FOR A POLYHARMONIC PROBLEM ON R n. Abdelwaheb Dhifli

( ) exp i ω b ( ) [ III-1 ] exp( i ω ab. exp( i ω ba

Effect of Wall Absorption on dispersion of a solute in a Herschel Bulkley Fluid through an annulus

Monochromatic Wave over One and Two Bars

Elastic-Plastic Deformation of a Rotating Solid Disk of Exponentially Varying Thickness and Exponentially Varying Density

Representing Knowledge. CS 188: Artificial Intelligence Fall Properties of BNs. Independence? Reachability (the Bayes Ball) Example

For demonstration of the concept of HAM, by considering general non-linear problem (1) Non-linear operator is N and v (t) [ ],

156 There are 9 books stacked on a shelf. The thickness of each book is either 1 inch or 2

Application of variational iteration method for solving the nonlinear generalized Ito system

Positive continuous solution of a quadratic integral equation of fractional orders

CS 188: Artificial Intelligence Fall Probabilistic Models

Feedback Couplings in Chemical Reactions

1 Widrow-Hoff Algorithm

Discretization of Fractional Order Differentiator and Integrator with Different Fractional Orders

On the approximation of particular solution of nonhomogeneous linear differential equation with Legendre series

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Chapter Finite Difference Method for Ordinary Differential Equations

The Homotopy Analysis Method for Solving Multi- Fractional Order Integro- Differential Equations

18 Biological models with discrete time

Stochastic Model for Cancer Cell Growth through Single Forward Mutation

Design Considerations for Achieving ZVS in a Half Bridge Inverter that Drives a Piezoelectric Transformer with No Series Inductor

A GENERAL METHOD TO STUDY THE MOTION IN A NON-INERTIAL REFERENCE FRAME

A FINITE-MEMORY DISCRETE-TIME CONVOLUTION APPROACH FOR THE NON-LINEAR DYNAMIC MODELLING OF S/H-ADC DEVICES

Chapter 7 Response of First-order RL and RC Circuits

Ordinary Differential Equations

A PREY-PREDATOR MODEL WITH AN ALTERNATIVE FOOD FOR THE PREDATOR AND OPTIMAL HARVESTING OF THE PREDATOR

On a Class of Two Dimensional Twisted q-tangent Numbers and Polynomials

A New Perturbative Approach in Nonlinear Singularity Analysis

Application of homotopy perturbation method to the Navier-Stokes equations in cylindrical coordinates

Fourier Series & The Fourier Transform. Joseph Fourier, our hero. Lord Kelvin on Fourier s theorem. What do we want from the Fourier Transform?

Transcription:

Available online a www.pelagiaeseachlibay.co Advances in Applied Science Reseach,, 3 (3):8-86 A Maheaical sudy of Two Species Aensalis Model Wih a Cove fo he fis Species by Hooopy Analysis Mehod B. Sia Rababu, K. L. Naayan and Shahanaz Bahul 3 ISSN: 976-86 CODEN (USA): AASRFC Depaen of Basic sciences & Huaniies.AVN Insiue of Engineeing & Technology, Hyd Depaen of Basic sciences & Huaniies.SLC Insiue of Engineeing & Technology, Hyd 3 Depaen of Basic sciences & Huaniies. JNT Univesiy, Kukapally, Hyd _ ABSTRACT The pesen pape is devoed o an analyical invesigaion of a wo species aensalis odel wih a paial cove fo he fis species o poec i fo he second species. The seies soluion of he non-linea syse was appoxiaed by he Hooopy analysis ehod (HAM) and he soluions ae suppoed by nueical exaples. Key Wods: Aensalis, zeo ode defoaion, ebedding paaee, linea opeao, Non linea opeao and HAM. _ INTRODUCTION Sybioses ae a boad class of ineacions aong oganiss --aensalis involves one ogais affecing anohe negaively wihou any posiive o negaive benefi fo iself. A. V. N. Achayulu and Paabhi Raachayulu [,,3,4] sudied he sabiliy of eney aensal species pai wih liied esouces and B. Shiva Pakash and T. Kaunanihi sudied he ineacion beween schizosacchaoyces pobe and sacchaoyces ceevisiae o pedic sable opeaing condiions in a cheosa [5].. Abou HAM: In 99 Liao eployee he basic idea of hooopy in opology o popose a poweful analyical ehod fo nonlinea pobles naely Hooopy Analysis Mehod [6,7,8,9,]. Lae on M. Ayub, A. Rasheed, T. Haya, Fadi & Awawdeh [,,3] successfully applied his echnique o solve diffeen ypes of non-linea pobles. The HAM iself povides us wih a convenien way o conol adjus he convegence egion and ae of appoxiaion seies. In his pape we popose HAM ehod o invesigae he seies soluions of a wo species aensalis odel wih a cove fo he fis species o poec i fo he aacks of he second species. Exaples: Aavian boulis and ed ides (caused by dino flagellaes) ae ofen exeely oxic fo bids, aine aals, huans; ec. Aensalis ay lead o he pe-epive colonizaion of a habia. Once an oganis esablishes iself wihin a habia i ay peven ohe populaions fo suviving in ha habia. The poducion of lacic acid o siila low-olecula-weigh fay acids is inhibioy o any baceial populaions. Populaions able o poduce and oleae high concenaions of lacic acids, fo exaple, ae able o odify he habia so as o peclude he gowh of ohe baceial populaions. E.coli is unable o gow in he uen, pobably because of he pesence of volaile fay acids poduced hee by anaeobic heeoophic icobial populaions. Fay acids 8

B. Sia Rababu e al Adv. Appl. Sci. Res.,, 3(3):8-86 poduced by icooganiss on skin sufaces ae believed o peven he colonizaion of hese habias by ohe icooganiss. Populaions of yeass on skin sufaces ae ainained in low nubes by icobial populaions poducing fay acids. Acids poduced by icobial populaions in he vaginal ac ae pobably esponsible fo pevening infecion by pahogens such as Candida albicans. In he pesen invesigaion a wo species aensalis odel wih liied esouces fo boh he species and a paial cove fo he fis species o poec i fo he aacks of he second species was aken up fo analyic sudy. The odel is epesened by coupled non-linea odinay diffeenial equaions. The seies soluion of he non-linea syse is appoxiaed by Hooopy Analysis Mehod suppoed by nueical exaples. The govening equaions of he syse ae as follows dx = ax( ) αx ( ) α( k) x( ) y( ) dy = a y y ( ) α ( ) (.) Wih he noaion x(),y() ae especively he populaions of species and species, and k is a cove povided fo he species <k<. Basic ideas of HAM: In his pape, we apply he hooopy analysis ehod o he discussed poble. To show he basic idea, le us conside he following diffeenial equaion N(u,) =, (.) Whee N is a nonlinea opeao, denoe independen vaiable, u () is an unknown funcion, especively. Fo sipliciy, we ignoe all bounday o iniial condiions, which can be eaed in he siila way. By eans of genealizing he adiional hooopy ehod, Liao consucs he so-called zeo-ode defoaion equaion ( p) L[ φ( ; p) u ( )] = phh ( ) N[ φ( ; p)], (.) Whee p [,] is he ebedding paaee, h is a nonzeo auxiliay, paaee H is an auxiliay,paaee H is an auxiliay funcion L is an auxiliay linea opeao, u () is an iniial guess of u(),φ(,p) is a unknown funcion, especively. I is ipoan ha one has gea feedo o choose auxiliay hings in HAM. Obviously, When P= and p=, i holds φ (, ) = u (), φ (, ) = u () (.3) Respecively. Thus as p inceases fo o, he soluion φ (; p) vaies fo he iniial guesses u () o he soluion u(). Expanding φ(; p) in Taylo seies wih espec o p,one has φ( ; p) u ( ) u ( ) p Whee + = + (.4) = φ( ; p) u( ) =! p p= If he iniial guess (.3),he auxiliay linea paaee L i,he non-zeo auxiliay paaee h i and he auxiliay funcion H i ae popely choosen,so ha he powe seies (.4) conveges a p=. (.5) 8

B. Sia Rababu e al Adv. Appl. Sci. Res.,, 3(3):8-86 Then we have unde hese assupions he soluion seies + u( ) u ( ) u ( ) = + (.6) = Which us be one of soluion s of oiginal non linea equaion, as poved by Liao [5].As h =- and H()=,Eq (.) becoes ( p) L[ φ( ; p) u ( )] + pn[ φ( ; p)] =, (.7) which is used osly in he hooopy peubaion ehod, wheeas he soluion obained diecly, wihou using Taylo seies which is explained by H. Jafai, M. Zabihi and M. Saidy [4] and J. H. He [5,6] and S. J. Liao [7] copae he HAM and HPM. Accoding o he definiion, he govening equaion can be deduced fo he zeoode defoaion equaion (.7). Define he veco u = { u u,... u } k, k Diffeeniaing Eq. (.7), ies wih espec o ebedding paaee p and hen seing p= and finally dividing he by!, we have he so-called h-ode defoaion equaion L[ u ( ) u ( )] hh ( ) R ( u ), χ = Whee N[ φ( ; p)] R ( u ) =, ( )! p and p=,, χ =, >. (.9) 3. Applicaion: Conside he nonlinea diffeenial equaion(.) wih iniial condiions.we assue he soluion of he syse(.),x(),y() can be expessed by following se of base funcions in he fo + + (3.) = = x( ) = a, y( ) = b Whee a,b ae coefficiens o be deeined. This povides us he so called ule of soluion expession i.e., he soluion of (.) us be expessed in he sae fo as (3.) and he ohe expessions us be avoided. Accoding o (.) and (3.) we chose he linea opeao. To solve he syse of Eqs.(.),Hooopy analysis ehod is eployed. We conside he following iniial appoxiaions x ( ) = x( = ) = x y ( ) = y( = ) = y (3.) The linea and non-linea opeaos ae denoed as follows. dx( ; p) dy( ; p) L[ x( ; p)], L[ y( ; p)], (3.3) dx( ; p) N[ x(, p)] = a x( ; p) + αx ( ; p) + α( k) x( ; p) y( ; p) (3.4) (.8) 83

B. Sia Rababu e al Adv. Appl. Sci. Res.,, 3(3):8-86 dy( ; p) N [ y(, p)] = a y( ; p) + α y ( ; p) (3.5) Using above definiion he zeo ode defoaion equaion can be consuced as ( p) L [ x( ; p) x ( )] = ph N [ x, y],( p) L [ y( ; p) y ( )] = ph N [ x, y] (3.6) When p= and p=,fo he zeo-defoaion equaions one has, x( ;) = x ( ) x( ;) = x( ), y( ;) = y ( ) y( ;) = y( ) And expanding x(;p) and y(;p) in Taylos seies, wih espec o ebedding paaee p, one obains + + (3.8) = = x( ; p) = x ( ) + x ( ) p, y( ; p) = y ( ) + y ( ) p Whee d x( ; p) d y( ; p) x ( ) =, y ( ) = (3.9)! dp! dp p= p= + + p = { x ( ) = x ( ) + x ( ), y ( ) = y ( ) + y ( ) = = (3.7) (3.) Define he veco x = [ x ( ), x ( ),... x ( )], y = [ y ( ), y ( ),... y ( )] (3.) And apply he pocedue saed befoe. The following h -ode defoaion Eq will be achieved. L[ x( ) χx ( )] = h H( ) R ( x, y ), (3.) L [ y ( ) χ y ( )] = h H ( ) R ( x, y ), Le us conside H ( ) = H ( ) = and he iniial condiions x ( ) = x( = ) = x y ( ) = y( = ) = y in above equaions d d R ( x, y ) = N[ x(, p)] = x ( ) a x + α x ( ) x ( ) + α ( k) x ( ) y ( ) n n n n ( )! dp n= n= d d R ( x, y ) = N[ y(, p)] = y ( ) a y + α y ( ) y ( ) (3.3) n n ( )! dp n= The following will be obained successively 84

B. Sia Rababu e al Adv. Appl. Sci. Res.,, 3(3):8-86 L ( x ( ) χx ( ) ) = h x ( ) ax ( ) + αx ( ) + α( k) x ( ) y( ) χ ( ) =, and, > ( ) L x ( ) = h ax ( ) + αx ( ) + α( k) x ( ) y( ) x ( ) = h ax + αx + α( k) x y L ( y( ) χy( ) ) = h y( ) a y( ) + α y ( ) ( ) L y( ) = h a y( ) + α y ( ) y( ) = h a y + α y L ( x ( ) χ x ( ) ) = h ( ) ( ) ( ) ( ) ( ) ( ) ( ) x a x + α x x + α k x y n n n n n = n = x ( ) = ( h + h ) M + a h M + α x h M + α ( k) y M + haα ( k) x whee M = a x + α x + α ( k) x y L y ( ( ) χ y ( ) ) = h ( ) ( ) ( ) ( ) y a y + α y y n n n = h y y ( ) = ( h + h ) a y + α y + ( a 3a α y + α y ) L ( x3 ( ) χ3x( ) ) = h x( ) a x ( ) + α xn ( ) x n( ) + α ( k) xn ( ) y n( ) n= n= x3 ( ) = ( + h )( h + h ) M + ( + h ) M + h α y( h + h ) M + α h x ( h + h )( a y + α y ) 3 3 + a h M + h αm x + αh M + hα h x y ( a 3a α y + α y ) + h hα M( a y + α y ) + h αm y 3 M = ah ( k) M + h αx M + α ( k) ym + hα α x ( k) y hα a x ( k) L ( y ( ) χ y ( ) ) = h y ( ) a y ( ) + α 3 3 n n n= y ( ) y ( ) y h k h k a h k h k y a h k h k y α h k 3 3 3 3( ) = ( + ) 3 + [( + ) 4 3 + 3α ] + 4 + α 4 + ( h + h ) 3 Whee 85

B. Sia Rababu e al Adv. Appl. Sci. Res.,, 3(3):8-86 k = a x + αx + αx y h x k = h a x y a x y h a y y + + + + + + k3 = ( h + h ) a y + α y ( α α )( α α ) α ( α ) h y k a a y y 4 = + ( 3 α α ) The hee es appoxiaion o he soluion will be consideed as x( ) x + x ( ) + x ( ) + x ( ) 3 y( ) y + y ( ) + y ( ) + y ( ) 3 REFERENCES [].Achayulu K.V.L.N. & Paabhi Raachayulu. N.Ch. In.J.Open pobles Cop.Mah (IJOPCM), Vol.3.No..pp.73-9., Mach. []. Achayulu K.V.L.N. & Paabhi Raachayulu. Inenaional jounal of copuaional Inelligence Reseach (IJCIR), Vol.6, No.3; pp.343-358, June. [3]. Achayulu K.V.L.N. & Paabhi Raachayulu. N.Ch; Inenaional Jounal of Applied Maheaical Analysis and Applicaions.vol 4,No,pp.49-6,July 9. [4]. Achayulu K.V.L.N. & Paabhi Raachayulu. N.Ch. ; On An Aensal-Eney Ecological Model Wih Vaiable Aensal Coefficien is acceped fo publicaion in Inenaional Jounal of Copuaional cogniion(ijcc),yang s Scienific Reseach Insiue, USA(in pess). [5] Shiva Pakash & T.Kaunanihi; Inenaional Jounal of Che. Tech Reseach Coden (USA). [6] S.J.Liao,The poposed hooopy analysis echnique fo he soluion of nonlinea pobles,phd hesis,shanghai Jiao Tong Univesiy 99. [7] S.J.Liao Beyond peubaion: inoducion o he hooopy analysis ehod.crc Pess, Boca Raon: Chapan & Hall (3) [8] S.J.Liao. Appl.Mah. Copa., 47(4), 499-53. [9] S.J.Liao. Appl Mah Copu.,69(5),86-94. [] S.J.Liao In J Hea Mass Tansfe.,.48(5),59-539. [] M.Ayub, A.Rasheed, T.Haya. In J Eng Sci..4(3), 9-3. [] T.Haya, M.Khan. Nonlinea Dyn.,4:(5),395-45. [3] Fadi Awawdeh, H.M. Jaada, O. Alsayyed, Solving syse of DAEs by hooopy analysis ehod, Chaos, Soluions and Facals 4 (9) 4 47,Elsevie. [4] H.Jafai, M.Zabihi and M.Saidy. Appl.Mah.sci.,, 8),393-396. [5] J.H.He. Phys Le A.35 ()(6),87-88. [6] J.H.He, Appl.Mah. Mehod, 4(4) 759-766. [7] SJ.Liao, Appl.Mah.Copu. 69 (5) 86-94. [9]Shiva Reddy. K and Paabhiaachayulu, N.Ch. Adv. Appl. Sci. Res.,,, 3, 8-8. [] R. Silaha, R. Ravinda Reddy & N.Ch Paabhiaachayulu, Adv. Appl. Sci. Res.,,, 3, 5-65 [] R. Silaha, & N.Ch Paabhiaachayulu, Adv. Appl. Sci. Res.,,, 3, 66-78 [] K. Madhusudhan Reddy and Lakshi Naayan.K Adv. Appl. Sci. Res.,,, 4, 45-459. [3] B. Hai Pasad and N.Ch Paabhiaachayulu, Adv. Appl. Sci. Res.,,, 5, 97-6. 86