(a) In order to simplify this part, let's introduce a change in the
notation.
Let
| Method | Original notation | Changes to |
|---|---|---|
| Newton | ei(2) = k2 (ei-1(2))2 | ei = k (ei-1)2 |
| Newton-Chord | ei = k (ei k3 (ei-1(3)) | Ei = K ei-1 |
A table of error contractions looks like the following:
| Iteration | Newton | Newton-Chord |
|---|---|---|
| 2 | k(e1)2 | Ke1 |
| 3 | k3(e1)4 | K2e1 |
| 4 | k7(e1)8 | K3e1 |
| 5 | k15(e1)16 | K4e1 |
| 6 | k31(e1)32 | K5e1 |
| 7 | k63(e1)64 | K6e1 |
| 8 | k127(e1)128 | K7e1 |
| 9 | k255(e1)256 | K8e1 |
(b) The first iteration is the same for both methods, namely
The rest of the iterations, the Newton method does the following:
The Newton-Chord method does the following:
Total Costs:
| Method> | Cost |
|---|---|
| Newton | C2L |
| Newton-Chord | (C3-1)M+L |
(c) Ignore the first iteration.
Without loss of generality, assume that C2 and C3
have been adjusted down by 1 each.
Then, without loss of generality, we must only compare
| N | C2 | |
|---|---|---|
| Small | Large | |
| Small | (*) | Newton |
| Large | Newton-Chord | (*) |
Cheers,
Craig C. Douglas