If you have homework to submit up to section 2.1,
please do so now.
Your 2.2 homework is due Friday: please scan it and
email, or drop it off at my office.
You have a new assignment for
section 2.3; hopefully you can get that to me by next Friday.
Questions on anything?
Let's recall what we did last time:
We finished up fixed point iterations with a few issues that had
arisen during our first discussion. In particular,
We talked some more about the "crumpet" about chaos, and
how to find the "bifurcation points", where period doubling
occurs in the oscillations. We found the first such place by
considering a new map, which was just an iterated map of :
.
I didn't mention our author's cobwebbing
animation, but you should take a look at that!
We considered changing the fixed point function that I
used for farcsine
(I used in my version, which struggles near in
the farcsine function.
We discovered that other values of couldn't solve
the problem, which is that at values of
near 1, and that's a problem for fixed point iteration.
Today:
Let's begin with any other questions about homework.
Then it's on to section 2.3
Do you like getting something for nothing? That's what we
seem to be doing in this section. Given a convergent sequence,
linearly convergent, we can accelerate its convergence using
its values.
Key points:
FPI is linear, unless at the fixed
point .
Proposition 5: Let be a differentiable function with fixed point
and let be an interval containing . If for all and , then for any initial
value , fixed point iteration, with for all
, gives an approximation of with absolute error no more than
.
FPI is quadratic if at the fixed
point .
Even though FPI may be linear, we can accelerate
it with just a little cleverness (Aitken's)!
We'll derive the method in two different ways.
Aitken's delta-squared method uses the starting
value and two successive iteratest to generate
an improved estimate. Steffensen's strategy was
then to use that improved estimate as the next
starting value, and then do it again:
and iterate....