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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

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