The Computable Differential Equation Lecture ... - Bruce E. Shapiro
The Computable Differential Equation Lecture ... - Bruce E. Shapiro
The Computable Differential Equation Lecture ... - Bruce E. Shapiro
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78 CHAPTER 4. IMPROVING ON EULER’S METHOD<br />
Figure 4.3: Numerical solution of equation 4.80 for h = 0.190 (red), h = 0.205<br />
(blue), and h = 0.23 (green).<br />
.<br />
Re(hλ) ≤ 0) then the method is said to be A-Stable. A-Stable methods are<br />
preferable for stiff problems. A stronger requirement is Stiff Decay: consider<br />
the generalized test equation<br />
y ′ = λ(y − g(t)) (4.85)<br />
where g(t) is any arbitrary, bounded function. <strong>The</strong>n we say that equation 4.85 has<br />
stiff decay if for any fixed t n > 0,<br />
lim |y n (t) − g(t n )| = 0. (4.86)<br />
hRe(λ)→−∞<br />
To determine the shape of this region we observe that in the complex plane we<br />
can write<br />
hλ = x + iy (4.87)<br />
and therefore<br />
1 ≥ |1 + x + iy| 2 (4.88)<br />
= (1 + x + iy)(1 + x − iy) 2 (4.89)<br />
= (1 + x) 2 + y 2 (4.90)<br />
which is a disk of radius 1 centered at the point (−1, 0).<br />
If λ ∈ R then this condition gives<br />
−1 ≤ 1 + hλ ≤ 1 (4.91)<br />
If λ < 0 then<br />
−2 ≤ hλ ≤ 0 (4.92)<br />
h ≤ − 2 λ<br />
(4.93)<br />
Math 582B, Spring 2007<br />
California State University Northridge<br />
c○2007, B.E.<strong>Shapiro</strong><br />
Last revised: May 23, 2007