Theory and Modern Applications
ε ↓∖ N → | 32 | 64 | 128 | 256 | 512 | 1,024 |
---|---|---|---|---|---|---|
2−5 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 1.967E − 06 |
2−6 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 7.480E − 07 |
2−7 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.579E − 07 |
2−8 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−9 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−10 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−11 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−12 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−13 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−14 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−15 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−16 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−17 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−18 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−19 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
2−20 | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
\(E^{N}\) | 1.017E − 05 | 5.086E − 06 | 2.543E − 06 | 1.272E − 06 | 6.358E − 07 | 5.544E − 07 |
\(R^{N}\) | 1.000E + 00 | 1.000E + 00 | 1.000E + 00 | 1.000E + 00 | 1.976E − 01 | 1.284E + 00 |