From the table below, we conclude that for , we have .
| | |
0 | 1 | 1.111 |
0.1 | 1.1110 | 1.2515307 |
0.2 | 1.2515307 | 1.4360575 |
0.3 | 1.4360575 | 1.6880074 |
0.4 | 1.6880074 | 2.0487708 |
0.5 | 2.0487708 | 2.6000252 |
From the table below, we conclude that for h = 0.05, we have
| | |
0 | 1 | 1.052625 |
0.05 | 1.052625 | 1.1113379 |
0.1 | 1.1113379 | 1.1774601 |
0.15 | 1.1774601 | 1.2526146 |
0.2 | 1.2526146 | 1.3388299 |
0.25 | 1.3388299 | 1.4386894 |
0.3 | 1.4386894 | 1.5555531 |
0.35 | 1.5555531 | 1.6938933 |
0.4 | 1.6938933 | 1.8598212
|
0.45 | 1.8598212 | 2.0619424 |
0.5 | 2.0619424 | 2.3128069 |
Therefore, for h = 0.1, we have and for h = 0.05, we have