| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 4 | 4.323 | 56/4:02.088 |
| 2 | 4 | 4.126 | 57/4:00.797 |
| 3 | 4 | 3.817 | 59/4:01.231 |
| 4 | 4 | 3.810 | 60/4:01.140 |
| 5 | 4 | 3.786 | 61/4:02.316 |
| 6 | 3 | 3.908 | 61/4:01.662 |
| 7 | 3 | 3.832 | 61/4:00.532 |
| 8 | 2 | 3.775 | 62/4:03.172 |
| 9 | 2 | 3.829 | 62/4:02.530 |
| 10 | 2 | 4.007 | 62/4:03.121 |
| 11 | 2 | 3.850 | 62/4:02.719 |
| 12 | 1 | 3.980 | 62/4:03.055 |
| 13 | 1 | 3.882 | 62/4:02.873 |
| 14 | 1 | 3.824 | 62/4:02.460 |
| 15 | 1 | 3.896 | 62/4:02.399 |
| 16 | 1 | 3.916 | 62/4:02.424 |
| 17 | 1 | 4.049 | 62/4:02.931 |
| 18 | 1 | 3.843 | 62/4:02.671 |
| 19 | 1 | 3.878 | 62/4:02.554 |
| 20 | 1 | 3.878 | 62/4:02.448 |
| 21 | 3 | 6.758 | 60/4:02.763 |
| 22 | 3 | 3.892 | 60/4:02.343 |
| 23 | 2 | 3.831 | 60/4:01.800 |
| 24 | 2 | 3.878 | 60/4:01.420 |
| 25 | 2 | 3.896 | 60/4:01.114 |
| 26 | 2 | 3.893 | 60/4:00.824 |
| 27 | 2 | 3.911 | 60/4:00.596 |
| 28 | 2 | 3.864 | 60/4:00.283 |
| 29 | 2 | 3.848 | 61/4:03.958 |
| 30 | 2 | 3.826 | 61/4:03.606 |
| 31 | 2 | 3.844 | 61/4:03.311 |
| 32 | 2 | 3.943 | 61/4:03.224 |
| 33 | 2 | 4.322 | 61/4:03.843 |
| 34 | 2 | 3.863 | 61/4:03.602 |
| 35 | 2 | 3.927 | 61/4:03.486 |
| 36 | 2 | 3.918 | 61/4:03.361 |
| 37 | 2 | 3.895 | 61/4:03.205 |
| 38 | 2 | 3.873 | 61/4:03.022 |
| 39 | 2 | 3.920 | 61/4:02.922 |
| 40 | 1 | 3.835 | 61/4:02.698 |
| 41 | 1 | 3.911 | 61/4:02.597 |
| 42 | 1 | 3.938 | 61/4:02.540 |
| 43 | 1 | 3.883 | 61/4:02.408 |
| 44 | 1 | 3.944 | 61/4:02.367 |
| 45 | 1 | 3.898 | 61/4:02.265 |
| 46 | 1 | 4.217 | 61/4:02.590 |
| 47 | 1 | 4.007 | 61/4:02.629 |
| 48 | 1 | 3.970 | 61/4:02.620 |
| 49 | 1 | 3.952 | 61/4:02.588 |
| 50 | 1 | 3.911 | 61/4:02.508 |
| 51 | 1 | 3.994 | 61/4:02.530 |
| 52 | 1 | 4.017 | 61/4:02.578 |
| 53 | 1 | 3.977 | 61/4:02.579 |
| 54 | 1 | 3.966 | 61/4:02.566 |
| 55 | 1 | 3.923 | 61/4:02.507 |
| 56 | 1 | 4.013 | 61/4:02.548 |
| 57 | 1 | 4.010 | 61/4:02.584 |
| 58 | 1 | 3.930 | 61/4:02.535 |
| 59 | 1 | 4.001 | 61/4:02.561 |
| 60 | 1 | 3.962 | 61/4:02.546 |
| 61 | 1 | 3.892 | 61/4:02.462 |