Theory and Modern Applications
α | h | τ | λ = 0 | \(\lambda=\frac {1}{100}\) | λ = 1 | |||
---|---|---|---|---|---|---|---|---|
∥ε(h,τ)∥ | Rate | ∥ε(h,τ)∥ | Rate | ∥ε(h,τ)∥ | Rate | |||
1.2 | \(\frac{1}{10}\) | \(\frac{1}{10}\) | 7.6335e − 04 | – | 7.5126e − 04 | – | 1.1638e − 03 | – |
\(\frac{1}{20}\) | \(\frac{1}{20}\) | 1.9911e − 04 | 1.9388 | 1.9631e − 04 | 1.9362 | 2.8958e − 04 | 2.0068 | |
\(\frac{1}{40}\) | \(\frac{1}{40}\) | 5.1544e − 05 | 1.9497 | 5.0882e − 05 | 1.9479 | 7.3198e − 05 | 1.9841 | |
\(\frac{1}{80}\) | \(\frac{1}{80}\) | 1.3313e − 05 | 1.9530 | 1.3155e − 05 | 1.9516 | 1.8860e − 05 | 1.9565 | |
\(\frac{1}{160}\) | \(\frac{1}{160}\) | 3.4300e − 06 | 1.9565 | 3.3923e − 06 | 1.9553 | 4.8865e − 06 | 1.9484 | |
1.5 | \(\frac{1}{10}\) | \(\frac{1}{10}\) | 9.6520e − 04 | – | 9.6198e − 04 | – | 2.4219e − 04 | – |
\(\frac{1}{20}\) | \(\frac{1}{20}\) | 2.3429e − 04 | 2.0425 | 2.3357e − 04 | 2.0421 | 6.6478e − 05 | 1.8652 | |
\(\frac{1}{40}\) | \(\frac{1}{40}\) | 5.6964e − 05 | 2.0402 | 5.6791e − 05 | 2.0401 | 1.8427e − 05 | 1.8510 | |
\(\frac{1}{80}\) | \(\frac{1}{80}\) | 1.3932e − 05 | 2.0317 | 1.3888e − 05 | 2.0318 | 5.2173e − 06 | 1.8205 | |
\(\frac{1}{160}\) | \(\frac{1}{160}\) | 3.4330e − 06 | 2.0208 | 3.4222e − 06 | 2.0209 | 1.4881e − 06 | 1.8099 | |
1.8 | \(\frac{1}{10}\) | \(\frac{1}{10}\) | 1.0924e − 03 | – | 1.0917e − 03 | – | 8.0464e − 04 | – |
\(\frac{1}{20}\) | \(\frac{1}{20}\) | 2.6152e − 04 | 2.0625 | 2.6141e − 04 | 2.0622 | 1.9630e − 04 | 2.0353 | |
\(\frac{1}{40}\) | \(\frac{1}{40}\) | 6.2776e − 05 | 2.0586 | 6.2754e − 05 | 2.0585 | 4.7153e − 05 | 2.0577 | |
\(\frac{1}{80}\) | \(\frac{1}{80}\) | 1.5082e − 05 | 2.0574 | 1.5077e − 05 | 2.0574 | 1.1234e − 05 | 2.0695 | |
\(\frac{1}{160}\) | \(\frac{1}{160}\) | 3.6282e − 06 | 2.0555 | 3.6268e − 06 | 2.0556 | 2.6688e − 06 | 2.0736 |