Theory and Modern Applications
ε ↓∖ N → | 32 | 64 | 128 | 256 | 512 | 1,024 |
---|---|---|---|---|---|---|
2−5 | 2.074E − 02 | 5.496E − 03 | 1.395E − 03 | 3.503E − 04 | 8.744E − 05 | 4.587E − 05 |
2−6 | 3.534E − 02 | 1.073E − 02 | 2.853E − 03 | 7.243E − 04 | 1.816E − 04 | 6.401E − 05 |
2−7 | 4.558E − 02 | 1.801E − 02 | 5.495E − 03 | 1.456E − 03 | 3.697E − 04 | 1.040E − 04 |
2−8 | 4.727E − 02 | 2.316E − 02 | 9.148E − 03 | 2.781E − 03 | 7.368E − 04 | 1.916E − 04 |
2−9 | 4.730E − 02 | 2.402E − 02 | 1.167E − 02 | 4.611E − 03 | 1.399E − 03 | 3.722E − 04 |
2−10 | 4.730E − 02 | 2.403E − 02 | 1.210E − 02 | 5.860E − 03 | 2.314E − 03 | 7.028E − 04 |
2−11 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.076E − 03 | 2.935E − 03 | 1.160E − 03 |
2−12 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.044E − 03 | 1.473E − 03 |
2−13 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.526E − 03 |
2−14 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
2−15 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
2−16 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
2−17 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
2−18 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
2−19 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
2−20 | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
\(E^{N}\) | 4.730E − 02 | 2.403E − 02 | 1.211E − 02 | 6.080E − 03 | 3.046E − 03 | 1.527E − 03 |
\(R^{N}\) | 9.769E − 01 | 9.886E − 01 | 9.941E − 01 | 9.972E − 01 | 9.965E − 01 | 1.002E + 00 |