ABSTRACT
In this thesis, the important fundamental properties of numerical methods for ordinary differential equations are investigated. This involves the derivation of Adams Bashforth methods, order and stability conditions and other basic concepts that are required to understand the methods.
TABLE
OF CONTENTS
Title Page i
Declaration ii
Certification iii
Dedication iv
Acknowledgement v
Table of Contents vi
List of figures
ix
List of tables x
Abstract xi
CHAPTER 1:
Introduction 1
1.1 Background of Study 1
1.2 Statement of the Problem 2
1.3 Aim and objectives 3
1.4 Significance of Study 3
1.5 Scope and Limitation 4
CHAPTER 2: LITERATURE REVIEW 6
CHAPTER 3: RESEARCH METHOD 8
3.1 Step Size 8
3.2 Mesh Size 8
3.3 One
Step Methods 8
3.4 Linear Multistep Methods (LMMs) 9
3.5
General K-Step Linear Multistep
Method 9
3.6 Lipschitz Condition 9
3.7 Existence and Uniqueness of Solution 10
3.8 Basis 10
3.9 Basis Function 10
3.10 Theorem 11
3.11 One Step Method 12
3.12 The
Euler Scheme 12
3.13 Runge-Kutta
Scheme 12
3.14 Linear
Multistep Method (LMM) 12
3.15 Families of Linear Multistep Method. 13
3.16 Adams-Bashforth 13
3.17 Adams – Moulton 13
3.18 Backward Differentiation Formula 13
3.19 Chebyshev Polynomials 14
3.20 Derivation
of Euler’s method 15
CHAPTER 4:
ANALYSIS OF METHODS 18
4.1. Introduction 18
4.2 Derivation of Adams Bashforth Method, when k = 2 19
4.3 Derivation of Adams Bashforth Method, when
k = 3 23
4.4 Derivation of Adams- Bashforth Method 26
4.5 Derivation of Adams-Bashforth Method 29
4.6 Consistency 32
4.7 Stability 32
4.8 Order and Error Estimation 38
4.9 Implementation
40
4.10 Numerical
Solution 42
4.11 Exact solution 42
Chapter 5: Summary, Conclusion and
Recommendation 48
5.1 Recommendation 48
REFERENCE
LIST OF FIGURES
Figure
4.1: The stability region for Adams Bashforth method for k=3 35
Figure
4.2: The Stability region for Adams Bashforth method for k=4 36
Figure
4.3: The Stability region for Adams Bashforth method for k=5 36
Figure
4.4: The Stability region for Adams Bashforth method for k=5 37
LIST
OF TABLES
Table 4.1Adams Bashforth Method for k=1 43
Table 4.2: Adams Bashforth method for K =2 43
Table 4.3: Adams Bashforth method for K =3 44
Table
4.4: Adams Bashforth method K= 4 44
Table 4.5: Adams Bashforh method for K =5 45
Table 4.6 45
Table 4.7:Error from Reformulated scheme 46
Table 4.8: Adam Bashforth Methods for k=3,
4, and 5 47
Table 4.9: Error from Adams Bashforth
methods for k=3,4 and 5 47
CHAPTER
1
Introduction
1.1 Background of Study
Numerical
methods are truly a crucial part of solving differential equations which cannot
be neglected since the late 18th century. Numerical methods for
solving differential equations have been developed continuously by many
Mathematicians Euler’s et al.,(1895).
According
to some historians of Mathematics, the study of differential equations began in
1675, when German Mathematician; Gottfried Leibniz wrote the following
equation:
The
attempt to solve physical problems led gradually to mathematical models
involving an equation in which a function and its derivatives play important
roles. However, the theoretical development of this new branch of mathematics,
Ordinary differential equations (ODE) has its origin rooted in a small number
of mathematical problems. These problems and their solutions led to independent
disciplines with the solutions of such equations an end in itself; however,
involving derivatives of only one independent variable are called ordinary
differential equations and may be classified as either initial value problem
(IVP) or boundary value
Problem
(BVP).
The
search for general methods of integrating differential equations began when
Isaac Newton (1642-1727) classified first order differential equation into
three classes.
Firstly,
ordinary derivative of one dependent variable with respect to a single
independent variable example
Secondly,
Ordinary
derivative of one or more dependent variables with respect to a single
independent variable example;
1.2 STATEMENT
OF THE PROBLEM
The methods of solving
higher order initial value problems (IVPs) of general Ordinary differential
equations by reduction order method has been reported to have difficulties in
computation, complication in writing computer programs and resultant wastage of
time.
Linear multistep methods
implemented by the predictor-Corrector mode have been found to be very
expensive to implement in times of the number of function evaluations per step,
the predictors often have lower order of accuracy than the correctors
especially when all the step and off step points are used for collocation and
interpolation, Asymptotically correct interpolation based spatial error by Tom
Arsenault.
In view of the
aforementioned problems, this work is motivated by the need to address the
setbacks associated with the existing methods, by considering the Adams
Bashforth methods. The methods are less expensive, in terms of the number of
functions evaluated per step. Also efficient in terms of accuracy and error term,
possess better rate of convergence and very easy to program resulting in
economy of computer time.
1.3 AIM
AND OBJECTIVES
The aim of this work is to
derive Adams Bashforth methods using Chebyshev polynomial as basis function. To
accomplish this aim, the following objectives were outlined:
i.
To derive
Adams Bashforth methods using Chebyshev polynomials
ii.
To implement the methods without the tedious
process of developing predictor separately.
iii.
To analyse basic properties of the methods
which include order, consistency zero stability, convergence and region of
absolute stability.
iv.
To test the performance of the methods for
accuracy and efficiency.
1.4 SIGNIFICANCE
OF STUDY
Conventional methods of
solving higher order initial value problems (IVP) of general ordianery
differential equation (ODE) by reduction order method has been reported to have
difficulties such as computational burden, complication in writing computer programs
and was of computer time (Awoyemi, 1992) and inability of the method to utilize
additional information associated with a specific ODEs such as the Oscillatory
nature of the solution (Vigo-Aguiar and Ramos, 2006).
Equivalently, linear
multistep methods implemented by the predictor-corrector mode have been found
to be very expensive to implement interms of the number of function evaluations
per step.
Hence the Adams Bashforth
method would be less expensive in terms of the number of functions evaluation
per step; highly efficient in terms of accuracy and error terms: flexible in
change of step size, posses better rate of convergence and weak stability
properties, and very easy to program resulting in economy of computer time.
1.5 SCOPE
AND LIMITATION
This work is limited to
the following:
1.
Only continuously differentiable functions
in the interval of integration were
considered
2.
The basis function considered in this work
is the Chebyshev polynomial
3.
The research work adopted only continuous
Adams Basthforth method
.
The
desire to obtain more accurate approximate solutions to mathematical models,
arising from science, engineering, and even social sciences in the form of
ordinary differential equations which do not have analytical solution has led
many scholars to propose several different numerical methods.
In
this chapter, some of the many contributions available in the literature are
reviewed. Specifically those numerical methods for the solution of ordinary
differential equations (ODE).
In
most applications, ordinary differential equations (ODEs) is solved by
reduction to an equivalent system of first order ordinary differential
equations of the form
For
any appropriate numerical method to be employed to solve the resultant system.
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