| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 3 | 4.003 | 60/4:00.180 |
| 2 | 3 | 3.758 | 62/4:00.591 |
| 3 | 3 | 3.847 | 63/4:03.768 |
| 4 | 2 | 3.962 | 62/4:01.335 |
| 5 | 2 | 3.800 | 62/4:00.188 |
| 6 | 2 | 3.848 | 63/4:03.789 |
| 7 | 2 | 3.816 | 63/4:03.306 |
| 8 | 2 | 3.842 | 63/4:03.148 |
| 9 | 2 | 3.887 | 63/4:03.341 |
| 10 | 2 | 3.808 | 63/4:02.997 |
| 11 | 2 | 3.816 | 63/4:02.762 |
| 12 | 2 | 3.764 | 63/4:02.293 |
| 13 | 2 | 3.832 | 63/4:02.225 |
| 14 | 2 | 3.816 | 63/4:02.096 |
| 15 | 2 | 4.327 | 62/4:00.254 |
| 16 | 2 | 4.078 | 62/4:01.041 |
| 17 | 2 | 4.216 | 62/4:02.238 |
| 18 | 2 | 4.012 | 62/4:02.599 |
| 19 | 2 | 3.723 | 62/4:01.979 |
| 20 | 2 | 3.970 | 62/4:02.188 |
| 21 | 2 | 4.118 | 62/4:02.813 |
| 22 | 2 | 4.248 | 62/4:03.747 |
| 23 | 2 | 3.706 | 62/4:03.140 |
| 24 | 2 | 3.991 | 62/4:03.319 |
| 25 | 2 | 3.922 | 62/4:03.313 |
| 26 | 2 | 3.804 | 62/4:03.026 |
| 27 | 2 | 3.818 | 62/4:02.792 |
| 28 | 2 | 3.930 | 62/4:02.823 |
| 29 | 2 | 3.861 | 62/4:02.704 |
| 30 | 2 | 3.826 | 62/4:02.521 |
| 31 | 2 | 3.841 | 62/4:02.380 |
| 32 | 2 | 3.758 | 62/4:02.087 |
| 33 | 2 | 3.924 | 62/4:02.123 |
| 34 | 2 | 3.799 | 62/4:01.929 |
| 35 | 2 | 3.925 | 62/4:01.970 |
| 36 | 2 | 3.934 | 62/4:02.024 |
| 37 | 2 | 3.780 | 62/4:01.817 |
| 38 | 2 | 3.765 | 62/4:01.596 |
| 39 | 2 | 3.944 | 62/4:01.671 |
| 40 | 2 | 3.827 | 62/4:01.561 |
| 41 | 2 | 3.853 | 62/4:01.496 |
| 42 | 2 | 3.772 | 62/4:01.314 |
| 43 | 2 | 3.870 | 62/4:01.282 |
| 44 | 2 | 3.899 | 62/4:01.293 |
| 45 | 2 | 3.812 | 62/4:01.183 |
| 46 | 2 | 4.004 | 62/4:01.336 |
| 47 | 2 | 3.758 | 62/4:01.159 |
| 48 | 2 | 4.041 | 62/4:01.354 |
| 49 | 2 | 3.888 | 62/4:01.348 |
| 50 | 2 | 4.423 | 62/4:02.006 |
| 51 | 2 | 3.870 | 62/4:01.965 |
| 52 | 2 | 3.989 | 62/4:02.068 |
| 53 | 2 | 6.694 | 61/4:01.375 |
| 54 | 2 | 4.212 | 61/4:01.663 |
| 55 | 2 | 4.179 | 61/4:01.904 |
| 56 | 2 | 3.841 | 61/4:01.768 |
| 57 | 2 | 3.943 | 61/4:01.746 |
| 58 | 2 | 4.036 | 61/4:01.823 |
| 59 | 2 | 3.819 | 61/4:01.673 |
| 60 | 2 | 3.844 | 61/4:01.553 |
| 61 | 2 | 3.899 | 61/4:01.492 |