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Numerical solution of Differential and Integral Equations

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Title: Numerical solution of Differential and Integral Equations


1
Numerical solution of Differential and Integral
Equations
  • PSCi702
  • October 19, 2005

2
Differential Equations
  • Equations where the dependent variable appears as
    well as one or more of its derivatives.
  • The highest derivative present determines the
    order of differential equation.
  • The highest power of the dependent variable or
    its derivative sets the degree of the
    differential equation.

3
Differential Equations
  • Y-Y0 (1st order)
  • Y(t)-Y(t)exp(t) (1st order)
  • Y(t)-Y(t)t2 (1st order)
  • YY-2Y0 (2nd order)
  • YY-2Y0 (3rd order)
  • YY20 ( 2nd degree, 1st order)
  • Y(t)(Y(t)-Y(t))2 t ( 2nd degree, 2nd order)

4
Differential Equations
  • Higher order equations can be reduced to a system
    of first order equations.

5
Differential Equations
  • When solving differential equations, the final
    answer has a constant of integration in it.
  • If all the constants of integrations are
    specified at the same place, they are then called
    initial values and the solution is called initial
    value problem.
  • If the initial values are not given at the same
    place and are specified at different locations,
    then the solution to the problem is called
    boundary value problem.

6
Solution to Differential Equations
  • Start the solution at the value of the
    independent variable for which the solution is
    equal to initial values.
  • Proceed step by step by changing the independent
    variable and obtaining solution across the
    required range.
  • Since most methods use local polynomial
    approximation methods, stability becomes an issue.

7
One Step Methods
  • Picards Method

8
Example
  • Use Picard iteration to find the solution of

9
Example
10
Example
  • The exact solution is

11
Runge-Kutta
  • The method doesnt rely on polynomial
    approximation.
  • Solution can be presented by a finite taylor
    series of the form

12
Runge-kutta
13
Runge-Kutta
14
Error Estimate
  • If solution is monotonically increasing, then the
    error is increasing as well due to truncation.
  • In oscillatory solutions, the truncation error
    introduces a phase shift.
  • The general accuracy can not be arbitrarily
    increased by decreasing the step size. While it
    will reduce the truncation error, it will
    increase the effects of round-off error.

15
Error Estimation
16
Example
17
Example
18
Example
19
Predictor-Corrector Method
  • By using the solution at n points, we can fit an
    (n-1) degree polynomial.
  • The predictor part extrapolates the solution over
    some finite range h based on the information at
    prior points and inherently unstable.
  • The corrector part makes correction at the end of
    the interval based on some prior information.

20
Predictor-Corrector Method
21
Predictor-Corrector Method
22
Predictor-Corrector Method
23
Systems of Differential Equations
24
Systems of Differential Equations
25
Systems of Differential Equations
  • In vector form
  • Where consists of elements which are
    functions of dependent variables yi,n and xn.
  • A set of basis solutions is simply a set of
    solutions, which are linearly independent.
  • Consider a set of m linear first order
    differential equations where k values of the
    dependent variables are specified at x0 and (m-k)
    values corresponding to the remaining dependent
    variables are specified at xn.

26
Systems of Differential Equations
  • solve (m-k) initial value problems starting at x0
    and specifying (m-k) independent, sets of missing
    initial values so that the initial value problems
    are uniquely determined. Let us denote the
    missing set of initial values at x0 by

27
  • The columns of are just the
    individual vectors
  • Matix A will have to be diagonal to always
    produce
  • So one can choose
  • So the missing initial values will be

28
Systems of Differential Equations
29
Integral Equations
  • Equations can be written where the dependent
    variable appears under an integral as well as
    alone.
  • Such equations are the analogue of the
    differential equations and are called integral
    equations.
  • It is often possible to turn a differential
    equation into an integral equation which may make
    the problem easier to numerically solve.

30
Integral Equations
31
Integral Equations
  • The parameter K(x,t) appearing in the integrand
    is known as the kernel of the integral equation.
  • Its form is crucial in determining the nature of
    the solution. Certainly one can have homogeneous
    or inhomogeneous integral equations depending on
    whether or not F(x) is zero. Of the two classes,
    the Fredholm are generally easier to solve.

32
Integral Equations
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