| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 5 | 5.951 | 41/4:03.991 |
| 2 | 5 | 3.935 | 49/4:02.207 |
| 3 | 5 | 3.906 | 53/4:03.659 |
| 4 | 5 | 3.853 | 55/4:02.619 |
| 5 | 4 | 4.081 | 56/4:03.331 |
| 6 | 4 | 3.665 | 57/4:01.214 |
| 7 | 4 | 3.636 | 58/4:00.509 |
| 8 | 4 | 3.622 | 59/4:00.786 |
| 9 | 4 | 4.240 | 59/4:01.828 |
| 10 | 4 | 3.988 | 59/4:01.174 |
| 11 | 4 | 3.590 | 60/4:02.547 |
| 12 | 4 | 3.569 | 60/4:00.180 |
| 13 | 4 | 3.704 | 61/4:02.780 |
| 14 | 4 | 3.685 | 61/4:01.495 |
| 15 | 4 | 4.513 | 61/4:03.748 |
| 16 | 4 | 3.546 | 61/4:02.033 |
| 17 | 4 | 3.691 | 61/4:01.040 |
| 18 | 4 | 4.943 | 60/4:00.393 |
| 19 | 4 | 3.533 | 61/4:02.880 |
| 20 | 4 | 3.556 | 61/4:01.581 |
| 21 | 4 | 3.550 | 61/4:00.389 |
| 22 | 4 | 3.498 | 62/4:03.082 |
| 23 | 4 | 3.564 | 62/4:02.121 |
| 24 | 4 | 3.592 | 62/4:01.312 |
| 25 | 4 | 3.495 | 62/4:00.327 |
| 26 | 4 | 3.746 | 62/4:00.016 |
| 27 | 4 | 3.676 | 63/4:03.432 |
| 28 | 4 | 4.068 | 62/4:00.020 |
| 29 | 4 | 3.682 | 63/4:03.480 |
| 30 | 4 | 3.711 | 63/4:03.157 |
| 31 | 4 | 3.954 | 63/4:03.349 |
| 32 | 4 | 3.629 | 63/4:02.889 |
| 33 | 4 | 3.863 | 63/4:02.903 |
| 34 | 4 | 5.040 | 62/4:01.207 |
| 35 | 4 | 4.742 | 62/4:02.716 |
| 36 | 4 | 4.111 | 62/4:03.054 |
| 37 | 4 | 3.515 | 62/4:02.375 |
| 38 | 4 | 3.656 | 62/4:01.962 |
| 39 | 4 | 3.988 | 62/4:02.097 |
| 40 | 4 | 3.785 | 62/4:01.912 |
| 41 | 4 | 3.444 | 62/4:01.219 |
| 42 | 4 | 3.611 | 62/4:00.807 |
| 43 | 4 | 3.852 | 62/4:00.760 |
| 44 | 4 | 3.612 | 62/4:00.378 |
| 45 | 4 | 3.725 | 62/4:00.169 |
| 46 | 4 | 3.664 | 63/4:03.755 |
| 47 | 4 | 3.587 | 63/4:03.377 |
| 48 | 4 | 6.305 | 62/4:02.668 |
| 49 | 5 | 4.583 | 62/4:03.514 |
| 50 | 4 | 3.969 | 62/4:03.566 |
| 51 | 4 | 3.764 | 62/4:03.366 |
| 52 | 4 | 3.789 | 62/4:03.203 |
| 53 | 4 | 3.741 | 62/4:02.991 |
| 54 | 4 | 4.435 | 62/4:03.583 |
| 55 | 4 | 5.166 | 61/4:01.027 |
| 56 | 4 | 4.684 | 61/4:01.825 |
| 57 | 4 | 3.742 | 61/4:01.587 |
| 58 | 4 | 4.826 | 61/4:02.497 |
| 59 | 4 | 3.821 | 61/4:02.337 |
| 60 | 4 | 4.159 | 61/4:02.527 |
| 61 | 4 | 3.941 | 61/4:02.492 |