Research Article | Open Access

Volume 2016 |Article ID 8921710 | https://doi.org/10.1155/2016/8921710

Susmita Paul, Sankar Prasad Mondal, Paritosh Bhattacharya, Kripasindhu Chaudhuri, "Some Comparison of Solutions by Different Numerical Techniques on Mathematical Biology Problem", International Journal of Differential Equations, vol. 2016, Article ID 8921710, 14 pages, 2016. https://doi.org/10.1155/2016/8921710

# Some Comparison of Solutions by Different Numerical Techniques on Mathematical Biology Problem

Accepted20 Oct 2016
Published07 Dec 2016

#### Abstract

We try to compare the solutions by some numerical techniques when we apply the methods on some mathematical biology problems. The Runge-Kutta-Fehlberg (RKF) method is a promising method to give an approximate solution of nonlinear ordinary differential equation systems, such as a model for insect population, one-species Lotka-Volterra model. The technique is described and illustrated by numerical examples. We modify the population models by taking the Holling type III functional response and intraspecific competition term and hence we solve it by this numerical technique and show that RKF method gives good results. We try to compare this method with the Laplace Adomian Decomposition Method (LADM) and with the exact solutions.

#### 1. Introduction

##### 1.1. Population Growth Model

Mathematical models of population growth have been formed to provide a significant angle of the real ecological situation. The meaning and importance of each parameter in the models have been defined biologically [1, 2]. In case of insect population, birth and death rate of a species typically are not constant; instead, they vary periodically with the passage of seasons, whereas the Lotka-Volterra equations demonstrate an arbitrary number of ecological competitors (or predator-prey) model which is dynamic in nature. The population growth model is very important in mathematical biology which is used basically to demonstrate a simple nonlinear control system in population growth.

##### 1.2. Holling Type III Functional Response

For getting exact population Holling type III functional response plays an important role in population dynamics. Holling type III functional response should be taken into the predator-prey interactions, which is proposed by Holling [3, 4] based on the fundament of experiment. The Holling type III functional response in ecological model is the intake rate of a predator species as a function of prey density.

##### 1.3. Numerical Techniques

In the field of science and technology, numerous significant physical phenomena are frequently modeled by nonlinear differential equations. Such equations are often very difficult to solve analytically. Yet, analytical approximate methods are very important for obtaining the accurate solutions which have gained much significance in recent years. There are various methods, undertaken to find out approximate solutions to nonlinear problems. Homotopy Perturbation Method (HPM), Homotopy Analysis Method (HAM), Differential Transform Method (DTM), Variational Iteration Method (VIM), Adomian Decomposition Method (ADM), Laplace Adomian Decomposition Method (LADM), and Runge-Kutta-Fehlberg (RKF) method are some very popular methods. The purpose of this paper is to bring out the numerical solution of various population models by using the approach, namely, Runge-Kutta-Fehlberg (RKF) method.

Recently, different scientists use the numerical method in their different problems. Here we try to give some references showing the importance of quasi-numerical methods techniques in present time: Kumar and Baskar  consider B-spline quasi-interpolation based numerical methods for some Sobolev type equations. Analytical and numerical study of dirty bosons in a quasi-one-dimensional harmonic trap is discussed by Khellil et al. . Numerical study of a quasi-hydrodynamic system of equations for flow computation at small Mach numbers is considered by Balashov and Savenkov . Quasi-optimal complexity of adaptive finite element method for linear elasticity problems in two dimensions is discussed by Liu et al. . Numerical solutions of quasi-two-dimensional models for laminar water hammer problems are considered by Zhao .

##### 1.4. Motivation

The accurate solutions of population growth models may become a difficult task if the equations are highly nonlinear. To overcome the situation there we take the numerical simulation, until there are no particular numerical methods for solving such problems. So to fill up the gap, here we find the approximated solutions of some population models by applying such some reliable, efficient, and more comfortable numerical technique (e.g., LADM, RKF) and try to conclude which one is the best.

##### 1.5. Novelties

The principal aim of this paper is to perform systematic analysis of the comparisons among exact solution and some reliable numerical techniques on the dynamics of the population model. The said numerical methods shall be more acceptable and reliable for solving such kind of problem. The issues which are addressed in the paper are described in the following:(i)Adding Holling type III functional response in insect population model and Lotka-Volterra model for better formulation(ii)Applying two numerical methods LADM and RKF for solution of the models and find the solution(iii)Analysis of the comparisons among exact solution, Laplace Adomian Decomposition Method (LADM), and Runge-Kutta-Fehlberg (RKF) method on the models(iv)The solution of the models by different numerical techniques being illustrated numerically and graphically(v)The necessary algorithm for numerical techniques givenMoreover, we can say all these developments can help the researchers who engage with nonlinear differential equation, mathematical biology, and numerical techniques.

##### 1.6. Structure of the Paper

The paper is organized as follows. The basic literature survey on population growth model, functional response, and numerical techniques is addressed in Section 1. In Section 2 we discuss the numerical methods, namely, Runge-Kutta-Felhberg (RKF) method and Laplace Adomian Decomposition Method (LADM) for nonlinear equation. The necessary algorithm for finding the numerical results is also discussed in this section. Section 3 is followed by a numerical example in different mathematical biology models. The different biological model is formulated and we write the general expression of the numerical solution. Section 4 is illustrated by the comparison study between the solutions and error terms of these said methods. Finally conclusions and future research scope of this paper are drawn in the last section, Section 5.

#### 2. Numerical Solution of Nonlinear Differential Equation

###### 2.1.1. LADM for Nonlinear Differential Equation

The Laplace Adomian Decomposition Method (LADM) [10, 11] was firstly introduced by Khuri and has been successfully used to find the solution of linear and nonlinear differential equations. The significant advantage of this method is that it is a combination of two powerful techniques, namely, Laplace transform and Adomian Decomposition Method . The Laplace transform is an elementary but useful technique for solving linear ordinary differential equations that is widely used by scientists and engineers for tackling the linear models. The main impotence of this method is that the solution of this method is expressed in -series which converges to the exact solution and will not take too much time for computing.

Consider the following nonlinear differential equation: where is a linear operator of the highest-order derivative which is assumed to be invertible easily, is the remaining linear operator of order less than and is a nonlinear operator, and is a source term.

Taking Laplace transform on both sides of the above equation, we getUsing the differential property of Laplace transform and using the initial condition, we getorNow we represent the unknown functions by an infinite series of the formHere the components are usually determined recurrently and the nonlinear operator can be decomposed into an infinite series of polynomials, given bywhere are Adomian polynomials of defined byTherefore,In general, the recursive relation is given byApplying the inverse Laplace transform to both sides of (9), we obtain  , , which is then substituted into (5).

For numerical computation, we get the expression as which is th term approximation of and the obtained series solution which converges to the exact solution.

###### 2.1.2. Algorithm for Finding the Numerical Solution by LADM

Step 1. Split the given equation into two parts. The first part isand the second part is

Step 2. Apply the Laplace transform to second part, determine the coefficient of , and solve this equation for . So, you can get .

Step 3. Calculate the Adomian polynomials for the function . Apply the Laplace transform to these polynomials.

Step 4. Divide the first part to the coefficient of . In a loop, calculate with substituting and into the first part.

Step 5. Construct the solution using inverse Laplace transform to .

Step 6. End

##### 2.2. Runge-Kutta-Fehlberg (RKF) Method
###### 2.2.1. RKF for Nonlinear Differential Equation

One of the most popular methods with a constant step size is the fourth-order Runge-Kutta (RK4) method. Reasonably the Runge-Kutta method can  obtain the accuracy of a Taylor Series approximation without the need of higher derivative calculations. This method can be considered as the basic form of other methods. However, in terms of error estimation, the one-step method with an adaptive step size like the Runge-Kutta-Fehlberg (RKF) method [17, 18] gives better error estimation than one-step method with a constant step size like the Runge-Kutta method. At each step the Runge-Kutta-Fehlberg method described the calculation of two Runge-Kutta methods of different order (RK4 and RK5). If the two answers are close enough then continue for the next step with the same step size. For a fixed accuracy the step size should be reduced. If the answers agree with more significant digits than required, the step size is increased. So we conclude that the one-step algorithm method associated with an adaptive step size automatically organizes the step size as a recomposition to the calculation truncation errors. This method has shown that it works in the case of nonlinear models and, hence, its application is found in wide range of deterministic and stochastic problems, linear and nonlinear problems, physics, biology, and chemical reactions problems, and so forth.

Consider the initial value problem The RKF is one way to try to resolve this problem.

The problem is to solve the initial value problem in the above equation by means of Runge-Kutta methods [19, 20] of order 4 and order 5.

First we need some definitions:Then an approximation to the solution of initial value problem is made using Runge-Kutta method of order 4:A better value for the solution is determined using a Runge-Kutta method of order 5:The numerical approximation of the global (local) discretization error at the point isIf , (where the maximum and minimum tolerance for local truncation error are and , respectively, which are prescribed at the beginning) then is an acceptable approximation of and the step size is considerable for the next step. Otherwise, the new step size can be determined by multiplying the scalar times the step size . The scalar is given bywhere is the specified error control tolerance.

Note. RK4 requires four functions for finding the result and RK5 requires six; that is total of ten for RK4 and RK5. Fehlberg devised a method to get RK4 and RK5 results using only six function evaluations by using some of values in both methods where .

###### 2.2.2. Algorithm for Finding the Numerical Solution by RKF

Step 1. “Function to be supplied”.

Step 2. Read , , , limit, .

Step 3. For limit

Step 4.

Step 5.

Step 6.

Step 7. Consider .

Step 8. . Write , .

Step 9. Repeat for better approximation.

Step 10. End the programme.

Step 11. Otherwise, with .

Step 12. Repeat Steps for better accuracy; any one can stop here. For better accuracy the process can be run.

#### 3. Solution of Some Population Model by Numerical Techniques

##### 3.1. Insect Population Model (Model I)

Suppose that an insect population shows the seasonal growth model which is discussed by Erbe et al. . The differential equation of the insect population model is given bywhere and are positive constants.

We now solve (23) by LADM with initial condition using the Laplace transform and Adomian Decomposition Method.Now, we have the following recursive algorithm by applying LADM,We now solve (23) by Runge-Kutta-Fehlberg (RKF) method.

Consider the initial value problem .

First we defineThen an approximation to the solution of initial value problem is made by using Runge-Kutta method of order 4:A better value for the solution is determined by using a Runge-Kutta method of order 5:

##### 3.2. Modified Insect Population Model (Model II)

Now we modify the above model by introducing Holling type III functional response which is defined in the following:The term is a Holling type III functional response, where and are positive constants and denotes the maximum capture rate of insects by a predator species.

The feeding rate saturates at the maximal feeding rate . This is intended to model that, for small densities, preys are able to evade predators by taking refuge. Such a functional response is known as sigmoidal. Biologically, a sigmoid functional response explains the fact that, at low densities of prey population, the effect of predation is low, but if the population size increases, predation is then more intensive. This phenomenon appears in a number of interactions in the real world and in this case it is said that the predator is generalist, because if the prey population size is low, it would then seek other food alternatives .

We now solve (29) by LADM with initial condition using the Laplace transform and Adomian Decomposition Method.

Now applying LADM, we have the following recursive algorithm:Therefore can be represented as a series and the Adomian Polynomial is calculating by formula given below:We now solve (29) by Runge-Kutta-Fehlberg (RKF) method.

Consider the initial value problem ,  .

First we defineThen an approximation to the solution of initial value problem is made by using Runge-Kutta method of order 4:A better value for the solution is determined by using a Runge-Kutta method of order 5:

##### 3.3. Introducing Interspecific Competition Term in Modified Insect Population Model (Model III)

Here we consider interspecific competition term in the insect population model. Interspecific competition is the most important aspect in the population growth dynamics model [23, 24]. It is assumed to be additional instantaneous deaths to the insect population and the increased death rate is proportional to the square of the predator density. This competition ennoble the death rate of the species; it is expected that the growth rate will considerably differ from the growth rate in a simple insect population model. Hence, we study the insect population model having interspecific competition in the population growth dynamics when either prey or predator or both the prey and predator populations are subject to harvest.where is the coefficient of interspecific competition term.

Solving (35) by LADM yields the following recursive algorithm:Therefore can be represented as a series and the Adomian Polynomial is calculating by formula given below:We now solve (35) by Runge-Kutta-Fehlberg (RKF) method.

Consider the initial value problem ,  .

First we defineThen an approximation to the solution of initial value problem is made by using Runge-Kutta method of order 4:A better value for the solution is determined by using a Runge-Kutta method of order 5:

##### 3.4. Lotka-Volterra Model

We define the Lotka-Volterra model into different ways as follows.

###### 3.4.1. Multispecies Lotka-Volterra Model

Mathematical models of population growth have been formed to provide an inconceivable significant angle of true ecological situation. The meaning of each parameter in the models has been defined biologically. For n species, we consider the following [25, 26] general Lotka-Volterra model: These equations may represent either predator-prey or competition cases.

###### 3.4.2. Single Species Lotka-Volterra Model (Model IV)

In case of one species, (41) is written for a given limited source of food:where and are positive constants. This equation has an exact solutionwhere is the initial condition.

Solving (42) by LADM yields the following recursive algorithm:where the Adomian Polynomials are given byWe now solve (42) by Runge-Kutta-Fehlberg (RKF) method.

Consider the initial value problem .

First we defineThen an approximation to the solution of initial value problem is made by using Runge-Kutta method of order 4:A better value for the solution is determined by using a Runge-Kutta method of order 5:

##### 3.5. Lotka-Volterra Equation with Holling Type III Functional Response (Model V)

Now we modify the Lotka-Volterra model by introducing Holling type III functional response which is defined asThe term is a Holling type III functional, where and are positive constants and denotes the predation rate and denotes half-saturation constant.

Solving (49) by LADM yields the following recursive algorithm:where the Adomian polynomials are given byWe now solve (49) by Runge-Kutta-Fehlberg (RKF) method:

Consider the initial value problem where we know thatThen an approximation to the solution of initial value problem is made by using Runge-Kutta method of order 4:A better value for the solution is determined using a Runge-Kutta method of order 5:

#### 4. Results and Discussion

The numerical solutions obtained by using the RKF, LADM method and are compared with the exact solution for different population models.

Remark 1. From Table 1 and Figure 1, we see the comparison among the RKF method, three-iterate LADM, and exact solutions for model I for particular numerical value of parameters and initial condition. The numerical results show that RKF method is of good accuracy.

 Exact solution Solution by RKF method Solution by LADM (three iterates) ERKF ELADM 0 1000.0000000 1000.0000000 1000.00000000 0.1 1217.4076457 1217.4447223 1216.07381402 0.2 1453.7920776 1453.8275070 1444.17894316 0.3 1673.5897680 1673.6084290 1647.56834151 0.4 1831.8331881 1831.8125036 1788.52160650 0.5 1889.5969624 1889.5159617 1838.84276708 0.6 1831.3776006 1831.2908389 1788.12230677 0.7 1672.7981525 1672.7809816 1646.85165910 0.8 1452.8457426 1452.9182247 1443.28432644 0.9 1216.4762073 1216.5807034 1215.15811427 1 999.1956876 999.2604905 999.19564898