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Title: OR682Math685CSI700


1
OR682/Math685/CSI700
  • Lecture 8
  • Fall 2000

2
Ordinary Differential Equations
  • Given an equation involving the derivatives of a
    function, solve for the function
  • True solution is a function we compute a finite
    approximation
  • Ordinary all derivatives are with respect to a
    single variable, often time

3
Boundary Conditions
  • Solve y? f (t,y) where t is a real variable,
    and f and y are vectors of length n
  • Solution is not unique
  • Boundary conditions must be specified
  • Initial value problem y (t0) y0
  • For example (1-dimensional)
  • y? y, y (t0) y0 y(t) y0et

Matlab functions ode15s Matlab m-files pop.m,
pop1.m
4
Higher-Order Problems
  • Equations with higher derivatives can be
    transformed to first-order problems
  • If u(n) f (t,u,u?,,u(n1)) we define y1 u,
    y2 u?, , yn(t) u(n 1)), so that

5
Example 2nd-order Equation
  • Falling object with air resistance (k constant)
  • Here g gravity, u height, v velocity
  • Transform to (y1 u(t), y2 u?(t))

Matlab m-files para.m, para1.m, pararun.m
6
Stability of ODEs
  • Unstable members of the solution family move
    apart with time errors are magnified
  • Stable members of the solution family move
    together with time errors reduced
  • Neutrally stable solution curves neither
    converge nor diverge
  • All forms of behavior can occur in a single
    problem as time varies

7
Measuring Stability
  • For the system y? f (t, y), stability is
    measured in terms of the Jacobian J fy
  • Look at the maximum of the real parts of the
    eigenvalues of J
  • Positive implies unstable
  • Negative implies stable
  • Zero implies neutrally stable
  • The Jacobian J changes with time

Matlab m-files stab_ex.m
8
Stability Linear System
  • Consider y? Ay, y(0) y0, for a matrix A
  • Let A have eigenvalues ?i with eigenvectors ui,
    and write y0 in the form
  • Then

9
Linear System (continued)
  • The Jacobian is J A
  • Eigenvalues of A with
  • positive real part yield exponentially growing
    components (unstable)
  • negative real part yield exponentially decaying
    components (stable)
  • Zero real part yield oscillatory components
    (neutrally stable)

Matlab m-files prey.m, prey1.m, runprey.m,
runprey1.m, ploteig.m, ploteig1.m
10
Numerical Solution of ODEs
  • Analytical solution formula (Matlab dsolve)
  • Numeric solution table of values
  • Starting at t0, the algorithm tracks the
    trajectory defined by the ODE
  • The ODE defines the slope of the trajectory
  • Use slope to predict y(t1)
  • Errors cause the estimates to lie on different
    curves in the solution family
  • If ODE unstable, errors are magnified as t
    increase

Matlab function dsolve Matlab m-file pop2.m
11
Eulers Method
  • Simple, but representative algorithm
  • Based on Taylor series approximation
  • Eulers method drop high-order terms

Matlab m-file eul.m
12
Types of Errors
  • Two distinct sources of error
  • Rounding due to finite precision of arithmetic
  • Truncation due to method used (formula is not
    exact, high-order terms are ignored)
  • Typically, truncation error is much larger than
    rounding error (many orders of magnitude larger)
  • We will ignore rounding error

13
Local Global Error
  • Truncation error comes in two forms
  • Local error made in one step of a numerical
    method (error in yk if yk1 were exact) Lk
  • Global total error in yk (local error plus
    effect of cumulative error) Ek yk y(tk)
  • Unstable equation global error will usually
    dominate
  • Stable equation local error will usually
    dominate
  • We can only control local error

14
Order of Numerical Method
  • A numerical method is said to have accuracy of
    order p if Lk O(h p1)
  • Reason a rough approximation of the global error
    is given by the sum of the local errors is
    proportional to h p1/ h h p

15
Analysis Eulers Method
  • Formulas for Taylor series Eulers method
  • Global error (consider 1-dimensional case)
  • Eulers method is a first-order method (letyk
    y(tk))

16
Growth Factor
  • Use the mean-value theorem to show that
  • for some unknown ?
  • Then (from our analysis above)
  • The global error is multiplied by the growth
    factor (1hk J)

17
Stability of Eulers Method
  • A numerical method is stable if small errors do
    not cause numerical solutions to diverge
  • Can be due to ODE itself
  • Eulers method is stable if the growth factor
    satisfies 1 h J lt 1
  • Equivalent to 2 lt h J lt 0

18
Stability (continued)
  • If equation is stable (J lt 0) then Eulers method
    is stable if 0 lt h lt 2 / J
  • For systems Eulers method is stable if the
    maximum real part of the eigenvalues of (I h
    J) is less than 1.

Matlab m-files runpreye.m, ploteige.m
19
Step-size Control
  • Have algorithm automatically choose h
  • Make h as large as possible
  • Maintain stability and accuracy
  • Based on estimates of local error, and stability
    analysis of algorithm
  • For Eulers method, local error is h2 y??/2, so

20
For Next Class
  • Homework see web site
  • Reading
  • Heath chapter 9 (rest of chapter)
  • Heath chapter 10
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