| Lap | Position | Time | Pace |
|---|---|---|---|
| 1 | 4 | 4.129 | 59/4:03.611 |
| 2 | 4 | 3.878 | 60/4:00.210 |
| 3 | 4 | 4.440 | 58/4:00.642 |
| 4 | 4 | 3.915 | 59/4:01.339 |
| 5 | 4 | 3.978 | 59/4:00.012 |
| 6 | 4 | 3.865 | 60/4:02.050 |
| 7 | 4 | 3.976 | 60/4:01.551 |
| 8 | 4 | 4.035 | 60/4:01.620 |
| 9 | 4 | 4.380 | 60/4:03.973 |
| 10 | 4 | 3.822 | 60/4:02.508 |
| 11 | 4 | 3.845 | 60/4:01.435 |
| 12 | 4 | 3.753 | 60/4:00.080 |
| 13 | 4 | 3.919 | 61/4:03.695 |
| 14 | 4 | 3.846 | 61/4:03.046 |
| 15 | 4 | 3.874 | 61/4:02.597 |
| 16 | 4 | 3.862 | 61/4:02.159 |
| 17 | 4 | 3.783 | 61/4:01.488 |
| 18 | 4 | 3.856 | 61/4:01.140 |
| 19 | 4 | 4.038 | 61/4:01.412 |
| 20 | 4 | 3.950 | 61/4:01.389 |
| 21 | 4 | 4.479 | 61/4:02.905 |
| 22 | 4 | 3.782 | 61/4:02.350 |
| 23 | 4 | 3.844 | 61/4:02.008 |
| 24 | 4 | 3.841 | 61/4:01.687 |
| 25 | 4 | 3.879 | 61/4:01.484 |
| 26 | 4 | 3.794 | 61/4:01.098 |
| 27 | 4 | 3.837 | 61/4:00.837 |
| 28 | 4 | 3.931 | 61/4:00.800 |
| 29 | 4 | 3.793 | 61/4:00.475 |
| 30 | 4 | 3.865 | 61/4:00.318 |
| 31 | 4 | 3.757 | 62/4:03.892 |
| 32 | 4 | 3.818 | 62/4:03.668 |
| 33 | 4 | 3.810 | 62/4:03.442 |
| 34 | 4 | 3.826 | 62/4:03.259 |
| 35 | 4 | 3.921 | 62/4:03.254 |
| 36 | 4 | 3.899 | 62/4:03.212 |
| 37 | 4 | 3.772 | 62/4:02.960 |
| 38 | 4 | 3.829 | 62/4:02.813 |
| 39 | 4 | 3.848 | 62/4:02.705 |
| 40 | 4 | 3.818 | 62/4:02.555 |
| 41 | 4 | 3.915 | 62/4:02.559 |
| 42 | 4 | 3.977 | 62/4:02.655 |
| 43 | 4 | 3.854 | 62/4:02.569 |
| 44 | 4 | 6.462 | 61/4:02.191 |
| 45 | 4 | 4.043 | 61/4:02.289 |
| 46 | 4 | 4.308 | 61/4:02.735 |
| 47 | 4 | 3.997 | 61/4:02.758 |
| 48 | 4 | 3.810 | 61/4:02.542 |
| 49 | 4 | 3.748 | 61/4:02.258 |
| 50 | 4 | 3.829 | 61/4:02.085 |
| 51 | 4 | 3.900 | 61/4:02.003 |
| 52 | 4 | 3.817 | 61/4:01.826 |
| 53 | 4 | 3.808 | 61/4:01.646 |
| 54 | 4 | 3.920 | 61/4:01.600 |
| 55 | 4 | 3.798 | 61/4:01.419 |
| 56 | 4 | 3.838 | 61/4:01.289 |
| 57 | 4 | 3.814 | 61/4:01.137 |
| 58 | 4 | 3.806 | 61/4:00.983 |
| 59 | 4 | 3.841 | 61/4:00.869 |
| 60 | 4 | 3.829 | 61/4:00.748 |
| 61 | 4 | 3.791 | 61/4:00.592 |