| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 4 | 4.558 | 53/4:01.574 |
| 2 | 4 | 3.918 | 57/4:01.566 |
| 3 | 3 | 4.024 | 58/4:01.667 |
| 4 | 3 | 4.082 | 58/4:00.439 |
| 5 | 3 | 3.797 | 59/4:00.472 |
| 6 | 3 | 3.717 | 60/4:00.960 |
| 7 | 3 | 3.847 | 61/4:03.503 |
| 8 | 3 | 7.367 | 55/4:02.756 |
| 9 | 3 | 3.922 | 56/4:04.110 |
| 10 | 3 | 3.604 | 57/4:04.165 |
| 11 | 3 | 3.632 | 57/4:00.789 |
| 12 | 3 | 3.797 | 58/4:02.947 |
| 13 | 3 | 3.668 | 58/4:00.624 |
| 14 | 3 | 3.660 | 59/4:02.713 |
| 15 | 3 | 3.835 | 59/4:01.617 |
| 16 | 3 | 3.700 | 59/4:00.159 |
| 17 | 3 | 3.718 | 60/4:02.986 |
| 18 | 3 | 3.745 | 60/4:01.970 |
| 19 | 3 | 3.872 | 60/4:01.462 |
| 20 | 3 | 4.034 | 60/4:01.491 |
| 21 | 3 | 3.806 | 60/4:00.866 |
| 22 | 3 | 3.819 | 60/4:00.333 |
| 23 | 3 | 4.073 | 60/4:00.509 |
| 24 | 3 | 3.797 | 61/4:03.980 |
| 25 | 3 | 3.796 | 61/4:03.483 |
| 26 | 3 | 3.914 | 61/4:03.301 |
| 27 | 3 | 3.771 | 61/4:02.809 |
| 28 | 3 | 3.739 | 61/4:02.283 |
| 29 | 3 | 3.857 | 61/4:02.042 |
| 30 | 3 | 3.739 | 61/4:01.576 |
| 31 | 3 | 3.889 | 61/4:01.436 |
| 32 | 3 | 3.729 | 61/4:01.000 |
| 33 | 3 | 3.756 | 61/4:00.639 |
| 34 | 3 | 3.725 | 61/4:00.245 |
| 35 | 3 | 3.732 | 62/4:03.818 |
| 36 | 3 | 3.773 | 62/4:03.543 |
| 37 | 3 | 3.719 | 62/4:03.192 |
| 38 | 3 | 3.846 | 62/4:03.068 |
| 39 | 3 | 3.799 | 62/4:02.875 |
| 40 | 3 | 3.739 | 62/4:02.598 |
| 41 | 3 | 3.751 | 62/4:02.353 |
| 42 | 3 | 3.757 | 62/4:02.129 |
| 43 | 3 | 3.755 | 62/4:01.912 |
| 44 | 3 | 3.764 | 62/4:01.718 |
| 45 | 3 | 3.779 | 62/4:01.553 |
| 46 | 3 | 4.067 | 62/4:01.784 |
| 47 | 3 | 3.761 | 62/4:01.601 |
| 48 | 3 | 3.749 | 62/4:01.410 |
| 49 | 3 | 3.907 | 62/4:01.427 |
| 50 | 3 | 3.748 | 62/4:01.246 |
| 51 | 3 | 3.849 | 62/4:01.195 |
| 52 | 3 | 3.764 | 62/4:01.044 |
| 53 | 3 | 3.831 | 62/4:00.978 |
| 54 | 3 | 7.543 | 61/4:01.221 |
| 55 | 3 | 3.802 | 61/4:01.052 |
| 56 | 3 | 3.802 | 61/4:00.889 |
| 57 | 3 | 3.890 | 61/4:00.826 |
| 58 | 3 | 3.797 | 61/4:00.667 |
| 59 | 3 | 3.772 | 61/4:00.488 |
| 60 | 3 | 3.780 | 61/4:00.323 |
| 61 | 3 | 4.007 | 61/4:00.390 |